From a6e96a188c323d06331c77063d0f7aabe1764038 Mon Sep 17 00:00:00 2001 From: DavideTisi Date: Wed, 13 Nov 2024 13:03:01 +0100 Subject: [PATCH 1/8] first commit --- docs/src/software/i-pi.sec | 1 + docs/src/topics/analysis.sec | 1 + examples/free-energy/README.rst | 2 + examples/free-energy/data.zip | Bin 0 -> 179081 bytes examples/free-energy/data/FES-md_hiq.bz2 | Bin 0 -> 38245 bytes examples/free-energy/data/FES-pimd_hiq.bz2 | Bin 0 -> 38190 bytes examples/free-energy/data/h5o2+.xyz | 9 + .../free-energy/data/h5o2.dms4B.coeff.com.dat | 993 ++++++++ .../free-energy/data/h5o2.pes4B.coeff.dat | 2022 +++++++++++++++++ examples/free-energy/data/input-md.xml | 73 + examples/free-energy/data/input-md_hiq.xml | 73 + examples/free-energy/data/input-pimd.xml | 74 + examples/free-energy/data/input-pimd_hiq.xml | 74 + examples/free-energy/data/plumed-md.dat | 10 + examples/free-energy/data/plumed-md_hiq.dat | 10 + examples/free-energy/data/plumed-pimd.dat | 10 + examples/free-energy/data/plumed-pimd_hiq.dat | 10 + examples/free-energy/environment.yml | 18 + examples/free-energy/free-energy.py | 50 + 19 files changed, 3430 insertions(+) create mode 100644 examples/free-energy/README.rst create mode 100644 examples/free-energy/data.zip create mode 100644 examples/free-energy/data/FES-md_hiq.bz2 create mode 100644 examples/free-energy/data/FES-pimd_hiq.bz2 create mode 100644 examples/free-energy/data/h5o2+.xyz create mode 100755 examples/free-energy/data/h5o2.dms4B.coeff.com.dat create mode 100755 examples/free-energy/data/h5o2.pes4B.coeff.dat create mode 100644 examples/free-energy/data/input-md.xml create mode 100644 examples/free-energy/data/input-md_hiq.xml create mode 100644 examples/free-energy/data/input-pimd.xml create mode 100644 examples/free-energy/data/input-pimd_hiq.xml create mode 100644 examples/free-energy/data/plumed-md.dat create mode 100644 examples/free-energy/data/plumed-md_hiq.dat create mode 100644 examples/free-energy/data/plumed-pimd.dat create mode 100644 examples/free-energy/data/plumed-pimd_hiq.dat create mode 100644 examples/free-energy/environment.yml create mode 100644 examples/free-energy/free-energy.py diff --git a/docs/src/software/i-pi.sec b/docs/src/software/i-pi.sec index 1ff3be9b..e7436f89 100644 --- a/docs/src/software/i-pi.sec +++ b/docs/src/software/i-pi.sec @@ -13,3 +13,4 @@ it on the `ipi-code website `_, the `documentation pages - examples/pi-metad/pi-metad - examples/heat-capacity/heat-capacity - examples/pi-mts-rpc/mts-rpc +- examples/free-energy/free-energy diff --git a/docs/src/topics/analysis.sec b/docs/src/topics/analysis.sec index a41e8820..2d56d7f9 100644 --- a/docs/src/topics/analysis.sec +++ b/docs/src/topics/analysis.sec @@ -7,3 +7,4 @@ for analysis or visualization purposes. - examples/gaas-map/gaas-map - examples/lpr/lpr - examples/roy-gch/roy-gch +- examples/free-energy/free-energy diff --git a/examples/free-energy/README.rst b/examples/free-energy/README.rst new file mode 100644 index 00000000..7525c6b2 --- /dev/null +++ b/examples/free-energy/README.rst @@ -0,0 +1,2 @@ +Free energy methods +=================== diff --git a/examples/free-energy/data.zip b/examples/free-energy/data.zip new file mode 100644 index 0000000000000000000000000000000000000000..180c78d78fe80901d63890a10133f9247177d8bb GIT binary patch literal 179081 zcmV(}K+wNXO9KQH0000008C_USpWb4000000000000jU50AyiwVJ}ci0|XQR000O8 zOk{0Y(v`?$Qi=coWt9K`6951JWMOn+FGfXEEp239XlZdSVtO)kdSy)kv+xh)_~}P;KoJJH{z$g-|O*aHvgCdq!Jr?a`KUPWzmD z?=O0uaqs^=zh-`apYLbBKjW9zPYs=YwABopptep%HQT>{a%+|`r|NY%*2oLDD zOY{2oKzGHB?AYuSVv%Mq&A^$L6=L*3mmx^m7il(E_+Ffk27y4}>@0*`*<}UbBS&Up zl|C7Crp!)2A(Kq3WUYhP^g;jaaR2%C2K=8S-@z=dpm!iu5F3c=|K9Km@Qeq6*jL_# zYJo1UM-D`99NHybesKp_=e!64X@Ni&f=i-LLBNRu(V`$p>31NI{-K`pX`|$QN9y*m{R0)rDd60hh>gKI!tAkh3pVo!k7&BATTZ*0b(%Xj#M&PHDVxShH4 z^2sUr%b+gKE)ZMvM(fMRRRGObqO~zN)|Ablix*&YM_AsdBvJo`63ZY0`@{pE^X7%0 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zundel
+
+ + data/h5o2+.xyz + data/plumed-md.dat + [doo, co1.lessthan, co2.lessthan, dc, mtd.bias ] + + 5000 + + positions{angstrom} + extras_bias + + [ step, time, conserved, temperature{kelvin}, kinetic_md, + potential, temperature{kelvin}(H), temperature{kelvin}(O), ensemble_bias ] + + + + 18885 + + + + + + + data/h5o2+.xyz + + [ 25.29166, 0, 0, 0, 25.29166, 0, 0, 0, 25.29166 ] + + + + 300.0 + + + + + + False + + 1.0 + + + + [ 8.191023526179e-4, 8.328506066524e-3, 1.657771834013e-3, 9.736989925341e-4, 2.841803794895e-4, -3.176846864198e-5, -2.967010478210e-4, + -8.389856546341e-4, 2.405526974742e-2, -1.507872374848e-2, 2.589784240185e-3, 1.516783633362e-3, -5.958833418565e-4, 4.198422349789e-4, + 7.798710586406e-4, 1.507872374848e-2, 8.569039501219e-3, 6.001000899602e-3, 1.062029383877e-3, 1.093939147968e-3, -2.661575532976e-3, + -9.676783161546e-4, -2.589784240185e-3, -6.001000899602e-3, 2.680459336535e-5, -5.214694469742e-5, 4.231304910751e-4, -2.104894919743e-5, + -2.841997149166e-4, -1.516783633362e-3, -1.062029383877e-3, 5.214694469742e-5, 1.433903506353e-9, -4.241574212449e-5, 7.910178912362e-5, + 3.333208286893e-5, 5.958833418565e-4, -1.093939147968e-3, -4.231304910751e-4, 4.241574212449e-5, 2.385554468441e-8, -3.139255482869e-5, + 2.967533789056e-4, -4.198422349789e-4, 2.661575532976e-3, 2.104894919743e-5, -7.910178912362e-5, 3.139255482869e-5, 2.432567259684e-11 + ] + + + + + + + [ plumed ] + + diff --git a/examples/free-energy/data/input-md_hiq.xml b/examples/free-energy/data/input-md_hiq.xml new file mode 100644 index 00000000..4208d757 --- /dev/null +++ b/examples/free-energy/data/input-md_hiq.xml @@ -0,0 +1,73 @@ + + + 1.00000000e-04
zundel
+
+ + data/h5o2+.xyz + data/plumed-md_hiq.dat + [doo, co1.lessthan, co2.lessthan, dc, mtd.bias ] + + 2000000 + + positions{angstrom} + extras_bias + + [ step, time, conserved, temperature{kelvin}, kinetic_md, + potential, temperature{kelvin}(H), temperature{kelvin}(O), ensemble_bias ] + + + + 18885 + + + + + + + data/h5o2+.xyz + + [ 25.29166, 0, 0, 0, 25.29166, 0, 0, 0, 25.29166 ] + + + + 300.0 + + + + + + False + + 0.5 + + + + [ 8.191023526179e-4, 8.328506066524e-3, 1.657771834013e-3, 9.736989925341e-4, 2.841803794895e-4, -3.176846864198e-5, -2.967010478210e-4, + -8.389856546341e-4, 2.405526974742e-2, -1.507872374848e-2, 2.589784240185e-3, 1.516783633362e-3, -5.958833418565e-4, 4.198422349789e-4, + 7.798710586406e-4, 1.507872374848e-2, 8.569039501219e-3, 6.001000899602e-3, 1.062029383877e-3, 1.093939147968e-3, -2.661575532976e-3, + -9.676783161546e-4, -2.589784240185e-3, -6.001000899602e-3, 2.680459336535e-5, -5.214694469742e-5, 4.231304910751e-4, -2.104894919743e-5, + -2.841997149166e-4, -1.516783633362e-3, -1.062029383877e-3, 5.214694469742e-5, 1.433903506353e-9, -4.241574212449e-5, 7.910178912362e-5, + 3.333208286893e-5, 5.958833418565e-4, -1.093939147968e-3, -4.231304910751e-4, 4.241574212449e-5, 2.385554468441e-8, -3.139255482869e-5, + 2.967533789056e-4, -4.198422349789e-4, 2.661575532976e-3, 2.104894919743e-5, -7.910178912362e-5, 3.139255482869e-5, 2.432567259684e-11 + ] + + + + + + + [ plumed ] + +
diff --git a/examples/free-energy/data/input-pimd.xml b/examples/free-energy/data/input-pimd.xml new file mode 100644 index 00000000..633cee81 --- /dev/null +++ b/examples/free-energy/data/input-pimd.xml @@ -0,0 +1,74 @@ + + + 1.00000000e-04
zundel
+
+ + data/h5o2+.xyz + data/plumed-pimd.dat + [doo, co1.lessthan, co2.lessthan, dc, mtd.bias ] + + 5000 + + positions{angstrom} + x_centroid{angstrom} + extras_bias + [ step, time, conserved, temperature{kelvin}, kinetic_cv, + potential, temperature{kelvin}(H), temperature{kelvin}(O), ensemble_bias ] + + + 18885 + + + + + + + data/h5o2+.xyz + + [ 25.29166, 0, 0, 0, 25.29166, 0, 0, 0, 25.29166 ] + + + + 300.0 + + + [ doo, dc, mtd.bias ] + + + + + False + + 1.0 + + + + [ 8.191023526179e-4, 8.328506066524e-3, 1.657771834013e-3, 9.736989925341e-4, 2.841803794895e-4, -3.176846864198e-5, -2.967010478210e-4, + -8.389856546341e-4, 2.405526974742e-2, -1.507872374848e-2, 2.589784240185e-3, 1.516783633362e-3, -5.958833418565e-4, 4.198422349789e-4, + 7.798710586406e-4, 1.507872374848e-2, 8.569039501219e-3, 6.001000899602e-3, 1.062029383877e-3, 1.093939147968e-3, -2.661575532976e-3, + -9.676783161546e-4, -2.589784240185e-3, -6.001000899602e-3, 2.680459336535e-5, -5.214694469742e-5, 4.231304910751e-4, -2.104894919743e-5, + -2.841997149166e-4, -1.516783633362e-3, -1.062029383877e-3, 5.214694469742e-5, 1.433903506353e-9, -4.241574212449e-5, 7.910178912362e-5, + 3.333208286893e-5, 5.958833418565e-4, -1.093939147968e-3, -4.231304910751e-4, 4.241574212449e-5, 2.385554468441e-8, -3.139255482869e-5, + 2.967533789056e-4, -4.198422349789e-4, 2.661575532976e-3, 2.104894919743e-5, -7.910178912362e-5, 3.139255482869e-5, 2.432567259684e-11 + ] + + + + + + + [ plumed ] + +
diff --git a/examples/free-energy/data/input-pimd_hiq.xml b/examples/free-energy/data/input-pimd_hiq.xml new file mode 100644 index 00000000..fa637ce0 --- /dev/null +++ b/examples/free-energy/data/input-pimd_hiq.xml @@ -0,0 +1,74 @@ + + + 1.00000000e-04
zundel
+
+ + data/h5o2+.xyz + data/plumed-pimd_hiq.dat + [doo, co1.lessthan, co2.lessthan, dc, mtd.bias ] + + 2000000 + + positions{angstrom} + x_centroid{angstrom} + extras_bias + [ step, time, conserved, temperature{kelvin}, kinetic_cv, + potential, temperature{kelvin}(H), temperature{kelvin}(O), ensemble_bias ] + + + 18885 + + + + + + + data/h5o2+.xyz + + [ 25.29166, 0, 0, 0, 25.29166, 0, 0, 0, 25.29166 ] + + + + 300.0 + + + [ doo, dc, mtd.bias ] + + + + + False + + 0.5 + + + + [ 8.191023526179e-4, 8.328506066524e-3, 1.657771834013e-3, 9.736989925341e-4, 2.841803794895e-4, -3.176846864198e-5, -2.967010478210e-4, + -8.389856546341e-4, 2.405526974742e-2, -1.507872374848e-2, 2.589784240185e-3, 1.516783633362e-3, -5.958833418565e-4, 4.198422349789e-4, + 7.798710586406e-4, 1.507872374848e-2, 8.569039501219e-3, 6.001000899602e-3, 1.062029383877e-3, 1.093939147968e-3, -2.661575532976e-3, + -9.676783161546e-4, -2.589784240185e-3, -6.001000899602e-3, 2.680459336535e-5, -5.214694469742e-5, 4.231304910751e-4, -2.104894919743e-5, + -2.841997149166e-4, -1.516783633362e-3, -1.062029383877e-3, 5.214694469742e-5, 1.433903506353e-9, -4.241574212449e-5, 7.910178912362e-5, + 3.333208286893e-5, 5.958833418565e-4, -1.093939147968e-3, -4.231304910751e-4, 4.241574212449e-5, 2.385554468441e-8, -3.139255482869e-5, + 2.967533789056e-4, -4.198422349789e-4, 2.661575532976e-3, 2.104894919743e-5, -7.910178912362e-5, 3.139255482869e-5, 2.432567259684e-11 + ] + + + + + + + [ plumed ] + +
diff --git a/examples/free-energy/data/plumed-md.dat b/examples/free-energy/data/plumed-md.dat new file mode 100644 index 00000000..6c839207 --- /dev/null +++ b/examples/free-energy/data/plumed-md.dat @@ -0,0 +1,10 @@ +# default units are LENGTH=nm ENERGY=kJ/mol TIME=ps +doo: DISTANCE ATOMS=1,2 +co1: DISTANCES GROUPA=1 GROUPB=3-7 LESS_THAN={RATIONAL R_0=0.14} +co2: DISTANCES GROUPA=2 GROUPB=3-7 LESS_THAN={RATIONAL R_0=0.14} +dc: COMBINE ARG=co1.lessthan,co2.lessthan COEFFICIENTS=1,-1 PERIODIC=NO +mtd: METAD ARG=doo,dc PACE=10 SIGMA=0.005,0.05 HEIGHT=4 FILE=HILLS-md BIASFACTOR=10 TEMP=300 +uwall: UPPER_WALLS ARG=doo AT=0.4 KAPPA=250 + +PRINT ARG=doo,co1.*,co2.*,dc,mtd.*,uwall.* STRIDE=10 FILE=COLVAR-md +FLUSH STRIDE=1 diff --git a/examples/free-energy/data/plumed-md_hiq.dat b/examples/free-energy/data/plumed-md_hiq.dat new file mode 100644 index 00000000..cc5a5302 --- /dev/null +++ b/examples/free-energy/data/plumed-md_hiq.dat @@ -0,0 +1,10 @@ +# default units are LENGTH=nm ENERGY=kJ/mol TIME=ps +doo: DISTANCE ATOMS=1,2 +co1: DISTANCES GROUPA=1 GROUPB=3-7 LESS_THAN={RATIONAL R_0=0.14} +co2: DISTANCES GROUPA=2 GROUPB=3-7 LESS_THAN={RATIONAL R_0=0.14} +dc: COMBINE ARG=co1.lessthan,co2.lessthan COEFFICIENTS=1,-1 PERIODIC=NO +mtd: METAD ARG=doo,dc PACE=100 SIGMA=0.0025,0.025 HEIGHT=1 FILE=HILLS-md_hiq BIASFACTOR=8 TEMP=300 +uwall: UPPER_WALLS ARG=doo AT=0.4 KAPPA=250 + +PRINT ARG=doo,co1.*,co2.*,dc,mtd.*,uwall.* STRIDE=20 FILE=COLVAR-md_hiq +FLUSH STRIDE=1 diff --git a/examples/free-energy/data/plumed-pimd.dat b/examples/free-energy/data/plumed-pimd.dat new file mode 100644 index 00000000..dcfd3478 --- /dev/null +++ b/examples/free-energy/data/plumed-pimd.dat @@ -0,0 +1,10 @@ +# default units are LENGTH=nm ENERGY=kJ/mol TIME=ps +doo: DISTANCE ATOMS=1,2 +co1: DISTANCES GROUPA=1 GROUPB=3-7 LESS_THAN={RATIONAL R_0=0.14} +co2: DISTANCES GROUPA=2 GROUPB=3-7 LESS_THAN={RATIONAL R_0=0.14} +dc: COMBINE ARG=co1.lessthan,co2.lessthan COEFFICIENTS=1,-1 PERIODIC=NO +mtd: METAD ARG=doo,dc PACE=10 SIGMA=0.005,0.05 HEIGHT=4 FILE=HILLS-pimd BIASFACTOR=10 TEMP=300 +uwall: UPPER_WALLS ARG=doo AT=0.4 KAPPA=250 + +PRINT ARG=doo,co1.*,co2.*,dc,mtd.*,uwall.* STRIDE=10 FILE=COLVAR-pimd +FLUSH STRIDE=1 diff --git a/examples/free-energy/data/plumed-pimd_hiq.dat b/examples/free-energy/data/plumed-pimd_hiq.dat new file mode 100644 index 00000000..3c8689c6 --- /dev/null +++ b/examples/free-energy/data/plumed-pimd_hiq.dat @@ -0,0 +1,10 @@ +# default units are LENGTH=nm ENERGY=kJ/mol TIME=ps +doo: DISTANCE ATOMS=1,2 +co1: DISTANCES GROUPA=1 GROUPB=3-7 LESS_THAN={RATIONAL R_0=0.14} +co2: DISTANCES GROUPA=2 GROUPB=3-7 LESS_THAN={RATIONAL R_0=0.14} +dc: COMBINE ARG=co1.lessthan,co2.lessthan COEFFICIENTS=1,-1 PERIODIC=NO +mtd: METAD ARG=doo,dc PACE=100 SIGMA=0.0025,0.025 HEIGHT=1 FILE=HILLS-pimd_hiq BIASFACTOR=8 TEMP=300 +uwall: UPPER_WALLS ARG=doo AT=0.4 KAPPA=250 + +PRINT ARG=doo,co1.*,co2.*,dc,mtd.*,uwall.* STRIDE=10 FILE=COLVAR-pimd_hiq +FLUSH STRIDE=1 diff --git a/examples/free-energy/environment.yml b/examples/free-energy/environment.yml new file mode 100644 index 00000000..05352af3 --- /dev/null +++ b/examples/free-energy/environment.yml @@ -0,0 +1,18 @@ +channels: + - plumed/label/nightly + - conda-forge +dependencies: + - python=3.11 + - pip + - gfortran + - make + - git + - plumed + - py-plumed + - pip: + - ase==3.22.1 + - git+https://github.com/i-pi/i-pi.git@main#egg=ipi + - matplotlib +variables: + PYTHONPATH: + PLUMED_KERNEL: diff --git a/examples/free-energy/free-energy.py b/examples/free-energy/free-energy.py new file mode 100644 index 00000000..adc4d8a0 --- /dev/null +++ b/examples/free-energy/free-energy.py @@ -0,0 +1,50 @@ +r""" +Free energy methods +========================== + +:Authors: Venkat Kapil `@venkatkapil24 `_ + and Davide Tisi `@DavideTisi `_ + +This example shows how to perform free energy calculation on a +effective Hamiltonian of a hydrogen atom in an effectively 1D double well +from Ref. `Y. Litman et al., JCP (2022) +`_ +""" + +# %% + +import os +import subprocess +import time + +import ipi.utils.parsing as pimdmooc +import numpy as np +import matplotlib.pyplot as plt + + + +# %% +# Model System +# ------------ +# +# We will consider the effective Hamiltonian of a hydrogen atom +# in an effectively 1D double well from +# Ref. `Y. Litman et al., JCP (2022) +# `_ +# Its potential energy surface (PES) is described by the function +# +# .. math:: +# +# V = A x^2 + B x^4 + \frac{1}{2} m \omega^2 y^2 + \frac{1}{2} m \omega^2 z^2 +# +# with: +# +# .. math:: +# +# \begin{align} +# m &= 1837.107~\text{a.u.}\\ +# \omega &= 3800 ~\text{cm}^{-1} = 0.017314074~\text{a.u.}\\ +# A &= -0.00476705894242374~\text{a.u.}\\ +# B &= 0.000598024968321866~\text{a.u.}\\ +# \end{align} +# From 79be02408fa873512f3af5c25a46753043344e33 Mon Sep 17 00:00:00 2001 From: DavideTisi Date: Wed, 13 Nov 2024 17:26:21 +0100 Subject: [PATCH 2/8] up to harmonic --- examples/free-energy/data.zip | Bin 179081 -> 0 bytes examples/free-energy/data/FES-md_hiq.bz2 | Bin 38245 -> 0 bytes examples/free-energy/data/FES-pimd_hiq.bz2 | Bin 38190 -> 0 bytes examples/free-energy/data/h5o2+.xyz | 9 - .../free-energy/data/h5o2.dms4B.coeff.com.dat | 993 -------- .../free-energy/data/h5o2.pes4B.coeff.dat | 2022 ----------------- examples/free-energy/data/input-md.xml | 73 - examples/free-energy/data/input-md_hiq.xml | 73 - examples/free-energy/data/input-pimd.xml | 74 - examples/free-energy/data/input-pimd_hiq.xml | 74 - examples/free-energy/data/plumed-md.dat | 10 - examples/free-energy/data/plumed-md_hiq.dat | 10 - examples/free-energy/data/plumed-pimd.dat | 10 - examples/free-energy/data/plumed-pimd_hiq.dat | 10 - examples/free-energy/environment.yml | 1 + examples/free-energy/free-energy.py | 321 +++ 16 files changed, 322 insertions(+), 3358 deletions(-) delete mode 100644 examples/free-energy/data.zip delete mode 100644 examples/free-energy/data/FES-md_hiq.bz2 delete mode 100644 examples/free-energy/data/FES-pimd_hiq.bz2 delete mode 100644 examples/free-energy/data/h5o2+.xyz delete mode 100755 examples/free-energy/data/h5o2.dms4B.coeff.com.dat delete mode 100755 examples/free-energy/data/h5o2.pes4B.coeff.dat delete mode 100644 examples/free-energy/data/input-md.xml delete mode 100644 examples/free-energy/data/input-md_hiq.xml delete mode 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zundel
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- - data/h5o2+.xyz - data/plumed-md.dat - [doo, co1.lessthan, co2.lessthan, dc, mtd.bias ] - - 5000 - - positions{angstrom} - extras_bias - - [ step, time, conserved, temperature{kelvin}, kinetic_md, - potential, temperature{kelvin}(H), temperature{kelvin}(O), ensemble_bias ] - - - - 18885 - - - - - - - data/h5o2+.xyz - - [ 25.29166, 0, 0, 0, 25.29166, 0, 0, 0, 25.29166 ] - - - - 300.0 - - - - - - False - - 1.0 - - - - [ 8.191023526179e-4, 8.328506066524e-3, 1.657771834013e-3, 9.736989925341e-4, 2.841803794895e-4, -3.176846864198e-5, -2.967010478210e-4, - -8.389856546341e-4, 2.405526974742e-2, -1.507872374848e-2, 2.589784240185e-3, 1.516783633362e-3, -5.958833418565e-4, 4.198422349789e-4, - 7.798710586406e-4, 1.507872374848e-2, 8.569039501219e-3, 6.001000899602e-3, 1.062029383877e-3, 1.093939147968e-3, -2.661575532976e-3, - -9.676783161546e-4, -2.589784240185e-3, -6.001000899602e-3, 2.680459336535e-5, -5.214694469742e-5, 4.231304910751e-4, -2.104894919743e-5, - -2.841997149166e-4, -1.516783633362e-3, -1.062029383877e-3, 5.214694469742e-5, 1.433903506353e-9, -4.241574212449e-5, 7.910178912362e-5, - 3.333208286893e-5, 5.958833418565e-4, -1.093939147968e-3, -4.231304910751e-4, 4.241574212449e-5, 2.385554468441e-8, -3.139255482869e-5, - 2.967533789056e-4, -4.198422349789e-4, 2.661575532976e-3, 2.104894919743e-5, -7.910178912362e-5, 3.139255482869e-5, 2.432567259684e-11 - ] - - - - - - - [ plumed ] - - diff --git a/examples/free-energy/data/input-md_hiq.xml b/examples/free-energy/data/input-md_hiq.xml deleted file mode 100644 index 4208d757..00000000 --- a/examples/free-energy/data/input-md_hiq.xml +++ /dev/null @@ -1,73 +0,0 @@ - - - 1.00000000e-04
zundel
-
- - data/h5o2+.xyz - data/plumed-md_hiq.dat - [doo, co1.lessthan, co2.lessthan, dc, mtd.bias ] - - 2000000 - - positions{angstrom} - extras_bias - - [ step, time, conserved, temperature{kelvin}, kinetic_md, - potential, temperature{kelvin}(H), temperature{kelvin}(O), ensemble_bias ] - - - - 18885 - - - - - - - data/h5o2+.xyz - - [ 25.29166, 0, 0, 0, 25.29166, 0, 0, 0, 25.29166 ] - - - - 300.0 - - - - - - False - - 0.5 - - - - [ 8.191023526179e-4, 8.328506066524e-3, 1.657771834013e-3, 9.736989925341e-4, 2.841803794895e-4, -3.176846864198e-5, -2.967010478210e-4, - -8.389856546341e-4, 2.405526974742e-2, -1.507872374848e-2, 2.589784240185e-3, 1.516783633362e-3, -5.958833418565e-4, 4.198422349789e-4, - 7.798710586406e-4, 1.507872374848e-2, 8.569039501219e-3, 6.001000899602e-3, 1.062029383877e-3, 1.093939147968e-3, -2.661575532976e-3, - -9.676783161546e-4, -2.589784240185e-3, -6.001000899602e-3, 2.680459336535e-5, -5.214694469742e-5, 4.231304910751e-4, -2.104894919743e-5, - -2.841997149166e-4, -1.516783633362e-3, -1.062029383877e-3, 5.214694469742e-5, 1.433903506353e-9, -4.241574212449e-5, 7.910178912362e-5, - 3.333208286893e-5, 5.958833418565e-4, -1.093939147968e-3, -4.231304910751e-4, 4.241574212449e-5, 2.385554468441e-8, -3.139255482869e-5, - 2.967533789056e-4, -4.198422349789e-4, 2.661575532976e-3, 2.104894919743e-5, -7.910178912362e-5, 3.139255482869e-5, 2.432567259684e-11 - ] - - - - - - - [ plumed ] - -
diff --git a/examples/free-energy/data/input-pimd.xml b/examples/free-energy/data/input-pimd.xml deleted file mode 100644 index 633cee81..00000000 --- a/examples/free-energy/data/input-pimd.xml +++ /dev/null @@ -1,74 +0,0 @@ - - - 1.00000000e-04
zundel
-
- - data/h5o2+.xyz - data/plumed-pimd.dat - [doo, co1.lessthan, co2.lessthan, dc, mtd.bias ] - - 5000 - - positions{angstrom} - x_centroid{angstrom} - extras_bias - [ step, time, conserved, temperature{kelvin}, kinetic_cv, - potential, temperature{kelvin}(H), temperature{kelvin}(O), ensemble_bias ] - - - 18885 - - - - - - - data/h5o2+.xyz - - [ 25.29166, 0, 0, 0, 25.29166, 0, 0, 0, 25.29166 ] - - - - 300.0 - - - [ doo, dc, mtd.bias ] - - - - - False - - 1.0 - - - - [ 8.191023526179e-4, 8.328506066524e-3, 1.657771834013e-3, 9.736989925341e-4, 2.841803794895e-4, -3.176846864198e-5, -2.967010478210e-4, - -8.389856546341e-4, 2.405526974742e-2, -1.507872374848e-2, 2.589784240185e-3, 1.516783633362e-3, -5.958833418565e-4, 4.198422349789e-4, - 7.798710586406e-4, 1.507872374848e-2, 8.569039501219e-3, 6.001000899602e-3, 1.062029383877e-3, 1.093939147968e-3, -2.661575532976e-3, - -9.676783161546e-4, -2.589784240185e-3, -6.001000899602e-3, 2.680459336535e-5, -5.214694469742e-5, 4.231304910751e-4, -2.104894919743e-5, - -2.841997149166e-4, -1.516783633362e-3, -1.062029383877e-3, 5.214694469742e-5, 1.433903506353e-9, -4.241574212449e-5, 7.910178912362e-5, - 3.333208286893e-5, 5.958833418565e-4, -1.093939147968e-3, -4.231304910751e-4, 4.241574212449e-5, 2.385554468441e-8, -3.139255482869e-5, - 2.967533789056e-4, -4.198422349789e-4, 2.661575532976e-3, 2.104894919743e-5, -7.910178912362e-5, 3.139255482869e-5, 2.432567259684e-11 - ] - - - - - - - [ plumed ] - -
diff --git a/examples/free-energy/data/input-pimd_hiq.xml b/examples/free-energy/data/input-pimd_hiq.xml deleted file mode 100644 index fa637ce0..00000000 --- a/examples/free-energy/data/input-pimd_hiq.xml +++ /dev/null @@ -1,74 +0,0 @@ - - - 1.00000000e-04
zundel
-
- - data/h5o2+.xyz - data/plumed-pimd_hiq.dat - [doo, co1.lessthan, co2.lessthan, dc, mtd.bias ] - - 2000000 - - positions{angstrom} - x_centroid{angstrom} - extras_bias - [ step, time, conserved, temperature{kelvin}, kinetic_cv, - potential, temperature{kelvin}(H), temperature{kelvin}(O), ensemble_bias ] - - - 18885 - - - - - - - data/h5o2+.xyz - - [ 25.29166, 0, 0, 0, 25.29166, 0, 0, 0, 25.29166 ] - - - - 300.0 - - - [ doo, dc, mtd.bias ] - - - - - False - - 0.5 - - - - [ 8.191023526179e-4, 8.328506066524e-3, 1.657771834013e-3, 9.736989925341e-4, 2.841803794895e-4, -3.176846864198e-5, -2.967010478210e-4, - -8.389856546341e-4, 2.405526974742e-2, -1.507872374848e-2, 2.589784240185e-3, 1.516783633362e-3, -5.958833418565e-4, 4.198422349789e-4, - 7.798710586406e-4, 1.507872374848e-2, 8.569039501219e-3, 6.001000899602e-3, 1.062029383877e-3, 1.093939147968e-3, -2.661575532976e-3, - -9.676783161546e-4, -2.589784240185e-3, -6.001000899602e-3, 2.680459336535e-5, -5.214694469742e-5, 4.231304910751e-4, -2.104894919743e-5, - -2.841997149166e-4, -1.516783633362e-3, -1.062029383877e-3, 5.214694469742e-5, 1.433903506353e-9, -4.241574212449e-5, 7.910178912362e-5, - 3.333208286893e-5, 5.958833418565e-4, -1.093939147968e-3, -4.231304910751e-4, 4.241574212449e-5, 2.385554468441e-8, -3.139255482869e-5, - 2.967533789056e-4, -4.198422349789e-4, 2.661575532976e-3, 2.104894919743e-5, -7.910178912362e-5, 3.139255482869e-5, 2.432567259684e-11 - ] - - - - - - - [ plumed ] - -
diff --git a/examples/free-energy/data/plumed-md.dat b/examples/free-energy/data/plumed-md.dat deleted file mode 100644 index 6c839207..00000000 --- a/examples/free-energy/data/plumed-md.dat +++ /dev/null @@ -1,10 +0,0 @@ -# default units are LENGTH=nm ENERGY=kJ/mol TIME=ps -doo: DISTANCE ATOMS=1,2 -co1: DISTANCES GROUPA=1 GROUPB=3-7 LESS_THAN={RATIONAL R_0=0.14} -co2: DISTANCES GROUPA=2 GROUPB=3-7 LESS_THAN={RATIONAL R_0=0.14} -dc: COMBINE ARG=co1.lessthan,co2.lessthan COEFFICIENTS=1,-1 PERIODIC=NO -mtd: METAD ARG=doo,dc PACE=10 SIGMA=0.005,0.05 HEIGHT=4 FILE=HILLS-md BIASFACTOR=10 TEMP=300 -uwall: UPPER_WALLS ARG=doo AT=0.4 KAPPA=250 - -PRINT ARG=doo,co1.*,co2.*,dc,mtd.*,uwall.* STRIDE=10 FILE=COLVAR-md -FLUSH STRIDE=1 diff --git a/examples/free-energy/data/plumed-md_hiq.dat b/examples/free-energy/data/plumed-md_hiq.dat deleted file mode 100644 index cc5a5302..00000000 --- a/examples/free-energy/data/plumed-md_hiq.dat +++ /dev/null @@ -1,10 +0,0 @@ -# default units are LENGTH=nm ENERGY=kJ/mol TIME=ps -doo: DISTANCE ATOMS=1,2 -co1: DISTANCES GROUPA=1 GROUPB=3-7 LESS_THAN={RATIONAL R_0=0.14} -co2: DISTANCES GROUPA=2 GROUPB=3-7 LESS_THAN={RATIONAL R_0=0.14} -dc: COMBINE ARG=co1.lessthan,co2.lessthan COEFFICIENTS=1,-1 PERIODIC=NO -mtd: METAD ARG=doo,dc PACE=100 SIGMA=0.0025,0.025 HEIGHT=1 FILE=HILLS-md_hiq BIASFACTOR=8 TEMP=300 -uwall: UPPER_WALLS ARG=doo AT=0.4 KAPPA=250 - -PRINT ARG=doo,co1.*,co2.*,dc,mtd.*,uwall.* STRIDE=20 FILE=COLVAR-md_hiq -FLUSH STRIDE=1 diff --git a/examples/free-energy/data/plumed-pimd.dat b/examples/free-energy/data/plumed-pimd.dat deleted file mode 100644 index dcfd3478..00000000 --- a/examples/free-energy/data/plumed-pimd.dat +++ /dev/null @@ -1,10 +0,0 @@ -# default units are LENGTH=nm ENERGY=kJ/mol TIME=ps -doo: DISTANCE ATOMS=1,2 -co1: DISTANCES GROUPA=1 GROUPB=3-7 LESS_THAN={RATIONAL R_0=0.14} -co2: DISTANCES GROUPA=2 GROUPB=3-7 LESS_THAN={RATIONAL R_0=0.14} -dc: COMBINE ARG=co1.lessthan,co2.lessthan COEFFICIENTS=1,-1 PERIODIC=NO -mtd: METAD ARG=doo,dc PACE=10 SIGMA=0.005,0.05 HEIGHT=4 FILE=HILLS-pimd BIASFACTOR=10 TEMP=300 -uwall: UPPER_WALLS ARG=doo AT=0.4 KAPPA=250 - -PRINT ARG=doo,co1.*,co2.*,dc,mtd.*,uwall.* STRIDE=10 FILE=COLVAR-pimd -FLUSH STRIDE=1 diff --git a/examples/free-energy/data/plumed-pimd_hiq.dat b/examples/free-energy/data/plumed-pimd_hiq.dat deleted file mode 100644 index 3c8689c6..00000000 --- a/examples/free-energy/data/plumed-pimd_hiq.dat +++ /dev/null @@ -1,10 +0,0 @@ -# default units are LENGTH=nm ENERGY=kJ/mol TIME=ps -doo: DISTANCE ATOMS=1,2 -co1: DISTANCES GROUPA=1 GROUPB=3-7 LESS_THAN={RATIONAL R_0=0.14} -co2: DISTANCES GROUPA=2 GROUPB=3-7 LESS_THAN={RATIONAL R_0=0.14} -dc: COMBINE ARG=co1.lessthan,co2.lessthan COEFFICIENTS=1,-1 PERIODIC=NO -mtd: METAD ARG=doo,dc PACE=100 SIGMA=0.0025,0.025 HEIGHT=1 FILE=HILLS-pimd_hiq BIASFACTOR=8 TEMP=300 -uwall: UPPER_WALLS ARG=doo AT=0.4 KAPPA=250 - -PRINT ARG=doo,co1.*,co2.*,dc,mtd.*,uwall.* STRIDE=10 FILE=COLVAR-pimd_hiq -FLUSH STRIDE=1 diff --git a/examples/free-energy/environment.yml b/examples/free-energy/environment.yml index 05352af3..35f747cc 100644 --- a/examples/free-energy/environment.yml +++ b/examples/free-energy/environment.yml @@ -11,6 +11,7 @@ dependencies: - py-plumed - pip: - ase==3.22.1 + - chemiscope - git+https://github.com/i-pi/i-pi.git@main#egg=ipi - matplotlib variables: diff --git a/examples/free-energy/free-energy.py b/examples/free-energy/free-energy.py index adc4d8a0..9f941f5b 100644 --- a/examples/free-energy/free-energy.py +++ b/examples/free-energy/free-energy.py @@ -17,6 +17,9 @@ import subprocess import time +import ipi +import ase.io +import chemiscope import ipi.utils.parsing as pimdmooc import numpy as np import matplotlib.pyplot as plt @@ -48,3 +51,321 @@ # B &= 0.000598024968321866~\text{a.u.}\\ # \end{align} # +# Let's define a function to visualize the PES! +# + +def PES(x, y , z): + """ + PES from Ref. `Y. Litman et al., JCP (2022)` + """ + + A = -0.00476705894242374 + B = 0.000598024968321866 + k = 1837.107 * 0.017314074**2 + + return A * x**2 + B * x**4 + k * y**2 / 2 + k * z**2 / 2 + +# %% +# The PES, in three dimensions, can be drawn with xy contours +# (each contour corresponds to kB T with T = 300 K), for various z values. +# + +x = np.linspace(-3,3,21) +y = np.linspace(-0.5,0.5,21) + +X, Y = np.meshgrid(x, y) +Z = PES(X, Y, 0) + + +contour_levels = [np.min(Z) + 0.00095004347 * i for i in range(12)] + +plt.title(r'$V(x,y,0)$') +plt.xlabel(r'$x$ [a.u.]') +plt.ylabel(r'$y$ [a.u.]') +plt.contour(X, Y, Z, levels=contour_levels) +plt.show() + +# %% +# **Questions**: +# +# 1. Looking at the contours can you tell +# if delocalization of the system to its other minimum is +# a rare event with respect to the time scale of +# the system's vibrations? +# +# 2. Feel free to plot it for various z values. +# Does the plot change? What does it tell you +# about the coupling between the modes? +# +# + +# %% +# Calculating the free energy of a hamiltonian +# ============================================ +# +# The harmonic approximation +# -------------------------- +# +# The harmonic approximation to the PES is essentially +# a truncated Taylor series expansion to second +# order around one of its minima. +# :math:`V^{\text{harm}} = V(q_0) + \frac{2}{2} \left.\frac{\partial^2 V}{\partial q^2}\right|_{q_0} (q - q_0)^2` +# where :math:`q = (x,y,z)` +# is a position vector and :math:`q_0 = \text{arg min}_{q} V` is +# the position where the PES has a local minimum. +# +# Let's use the i-PI code to optimize the PES with respect to its position +# to find :math:`q_0` and :math:`V^{\text{harm}}`. +# + +# %% +# Step 1: fixed cell geometry optimization +# ---------------------------------------- +# +# To find :math:`q_0` we will use the fixed-cell geometry +# optimization feature of i-PI! The inputs are +# into the `geop` directory. +# +# You will find the i-PI input file. Have a look at the +# `input.xml` file and see if you can understand its various parts. +# +# The snippet that implements the geometry optimization feature is +# +# .. code-block:: xml +# +# +# +# +# 1e-5 +# 1e-5 +# 1e-5 +# +# +# +# +# +# In essence, the geometry optimization is implemented as a +# motion class. At every step instead of performing "dynamics" we will +# simply move towards a local minimum of the PES. There are +# many algorithms for locally optimizing high-dimensional functions; +# here we use the robust +# `BFGS `_ +# method. The tolerances set thershold values for changes in the energy, +# positions and forces, that are sufficient to deem an optimization converged. +# + +# %% +# Installing the Python driver +# +# i-PI comes with a FORTRAN driver, which however has to be installed +# from source. We use a utility function to compile it. Note that this requires +# a functioning build system with `gfortran` and `make`. + +ipi.install_driver() +# %% +# To perform a fixed-cell geomerty optimization +# the bash script command should look like: +# +# .. code-block:: bash +# +# i-pi geop/input.xml > log.i-pi $ +# sleep(5) +# i-pi-driver -u -h geop -m doublewell_1D & +# +# The same can be achieved from Python using `subprocess.Popen` + + +ipi_process = subprocess.Popen(["i-pi", "geop/input.xml"]) +time.sleep(5) # wait for i-PI to start +driver_process =subprocess.Popen( + ["i-pi-driver", "-u", "-h", "geop", "-m", "doublewell_1D"] + ) + +# %% +# If you run this in a notebook, you can go ahead and start loading +# output files *before* i-PI and lammps have finished running, by +# skipping this cell + +ipi_process.wait() +driver_process.wait() + +# %% +# +# The number of steps taken for an optimization calculation depends on +# the system (the PES), the optimization method, +# and the initial configuration. Here, +# we initialize the system from :math:`q = (2.0, 0.2, -0.5)` +# as seen in the `geop/init.xyz` file. +# +# You can analyze your optimization calculation by plotting +# the potential energy vs steps and confirm if the potential +# energy has indeed converged to the set threshold! +# +# The final frame of the `geop.pos_0.xyz` file gives +# with chemiscope we can wisualize the minimzation +# trajectory and its energies. +# + +geop_out,_geop = ipi.read_output('geop.out') +geop_traj = ipi.read_trajectory("geop.pos_0.xyz") + +chemiscope.show( + frames=geop_traj, + properties={ + "steps": { "values" : np.arange(len(geop_traj)), + "target" : "structure"}, + "U":{"values": geop_out['potential'], + "target" : "structure"}, + }, + settings=chemiscope.quick_settings( + x="steps", y="U", trajectory=True + ), + mode="structure", +) + +# %% +# Step 2: harmonic calculation +# ---------------------------- +# +# To compute the system's Hessian we will use the vibrations feature of i-PI. +# Go through the `input.xml` file. +# The snippet that implements the vibrations feature is +# +# .. code-block:: xml +# +# +# +# 0.001 +# 0.001 +# phonons +# none +# +# +# +# The system's Hessian is computed using the finite difference method. +# This approach approximates the ij-th element of the Hessian in terms +# of the forces acting at infinitisemally displaced positions around the minimum: +# +# .. math:: +# +# \frac{\partial^2 V}{\partial q^2}_{ij} \approx - \frac{1}{2 \epsilon} +# \left(\left.f_{i}\right|_{q_{j} + \epsilon} - \left.f_{i}\right|_{q_{j} +# - \epsilon} \right) +# +# At every step instead of performing "dynamics", we will displace a degree of +# freedom along :math:`\pm \epsilon` and estimate one row of the Hessian. `pos_shift` sets +# the value of :math:`\epsilon` while `asr` zeros out the blocks of the Hessian due to continuous +# symmetries (translations or rotations for solids or clusters). In this example, +# we set this option to `none` as our system doesn't possess any continuous symmetries. +# + +# %% +# The initial configuration for this calculation should correspond to an +# opitimized position. You can obtain this from the last frame of the geop trajectory. + +ase.io.write('init_harm.xyz',geop_traj,format='extxyz') + +# %% +# The `bash` command for this would be +# +# .. code-block:: bash +# +# i-pi harm/input.xml > log.i-pi $ +# sleep(5) +# i-pi-driver -u -h vib -m doublewell_1D & +# +# Again we will use `subprocess.Popen` + +ipi_process = subprocess.Popen(["i-pi", "harm/input.xml"]) +time.sleep(5) # wait for i-PI to start +driver_process =subprocess.Popen( + ["i-pi-driver", "-u", "-h", "vib", "-m", "doublewell_1D"] + ) + +# %% +# If you run this in a notebook, you can go ahead and start loading +# output files *before* i-PI and lammps have finished running, by +# skipping this cell + +ipi_process.wait() +driver_process.wait() + +# %% +# The Hessian can be recovered from the `harm.phonons.hess`file. +# You can use the snippet below to plot the harmonic approximation +# to the PES +# + +def PES_harm(x,y,z): + """ + Harmonic approximation to the PES from Ref. `Y. Litman et al., JCP (2022)` around + a local minimum. Note this function is only valid for the example! + """ + + return V0 + hess[0,0] * (x - q0[0])**2 / 2 + hess[1,1] * (y - q0[1])**2 / 2 + hess[2,2] * (z - q0[2])**2 / 2 + +hess = np.loadtxt('harm.phonons.hess', comments='#') +q0 = ipi.read_trajectory('init_harm.xyz')[0].positions[0] / 0.529177 +V0 = np.loadtxt('harm.out', ndmin=2)[0,1] + +x = np.linspace(-3,3,21) +y = np.linspace(-0.5,0.5,21) + +X, Y = np.meshgrid(x, y) + +contour_levels = [np.min(Z) + 0.00095004347 * i for i in range(12)] + +plt.title(r'$V(x,y,0)$') +plt.xlabel(r'$x$ [a.u.]') +plt.ylabel(r'$y$ [a.u.]') +plt.contour(X, Y, PES(X, Y, 0), levels=contour_levels) +plt.show() + +plt.title(r'$V^{\mathrm{harm}}(x,y,0)$') +plt.xlabel(r'$x$ [a.u.]') +plt.ylabel(r'$y$ [a.u.]') +plt.contour(X, Y, PES_harm(X, Y, 0), levels=contour_levels) +plt.show() + +# %% +# The harmonic calculation also gives us the frequency modes +# from the dynamical matrix (mass scaled hessian)! +# + +W2s = np.loadtxt('harm.phonons.eigval') +print ('Harmonic Frequencies') +for w2 in W2s: + print('%10.5f cm^-1'% (w2**0.5 * 219474)) + +# %% +# These frequencies can be used to calculate the quantum harmonic +# free energy of the system -- an approxiamtion to its true free energy! +# + +def quantum_harmonic_free_energy(Ws, T): + """ + Receives a list of frequencies in atomic units and the temperature + in Kelvin. Returns the system's harmonic free energy. + """ + + hbar = 1 + kB = 3.1668116e-06 + + return V0 + -kB * T * np.log(1 - np.exp(-hbar * Ws / (kB * T))).sum() + +print ('Quantum Harmonic free energy: %15.8f [a.u.]'% (quantum_harmonic_free_energy(W2s**0.5, 300))) +print ('Quantum Harmonic free energy: %15.8f [eV]'% (quantum_harmonic_free_energy(W2s**0.5, 300) * 27.211386)) +print ('Quantum Harmonic free energy: %15.8f [kJ/mol]' % (quantum_harmonic_free_energy(W2s**0.5, 300) * 2625.4996)) + +# %% +# +# The exact free energy for the system when localized in one of +# the wells is still around 0.65 kJ/mol off w.r.t the harmonic limit. +# + +F = -7.53132797e-05 + quantum_harmonic_free_energy(W2s**0.5, 300) + +print ('Exact Quantum free energy: %15.8f [a.u.]'% (F)) +print ('Exact Quantum free energy: %15.8f [eV]'% (F * 27.211386)) +print ('Exact Quantum free energy: %15.8f [kJ/mol]' % (F * 2625.4996)) + From ac15f6861d3cd0b524fa89be7563a3908837c38f Mon Sep 17 00:00:00 2001 From: DavideTisi Date: Wed, 13 Nov 2024 17:39:48 +0100 Subject: [PATCH 3/8] start anharmonic --- examples/free-energy/free-energy.py | 40 ++++++++++++++++++++++++++++- 1 file changed, 39 insertions(+), 1 deletion(-) diff --git a/examples/free-energy/free-energy.py b/examples/free-energy/free-energy.py index 9f941f5b..3368f911 100644 --- a/examples/free-energy/free-energy.py +++ b/examples/free-energy/free-energy.py @@ -291,7 +291,7 @@ def PES(x, y , z): driver_process.wait() # %% -# The Hessian can be recovered from the `harm.phonons.hess`file. +# The Hessian can be recovered from the `harm.phonons.hess` file. # You can use the snippet below to plot the harmonic approximation # to the PES # @@ -369,3 +369,41 @@ def quantum_harmonic_free_energy(Ws, T): print ('Exact Quantum free energy: %15.8f [eV]'% (F * 27.211386)) print ('Exact Quantum free energy: %15.8f [kJ/mol]' % (F * 2625.4996)) +# %% +# +# Harmonic to anharmonic +# ---------------------- +# +# Calculating free energies beyond the harmonic approximation is non-trivial. +# There exist a familty of methods that can solve the vibrational Schroedinger +# Equation by approximating the anharmonic component of the PES, yielding an amharmonic +# free energy. While highly effective for low-dimensional or mildly anharmonic systems, +# the method of resort for *numerically-exact amharmonic free energies* of solid and clusters +# is the thermodynamic integration method combined with the path-integral method +# ( for applications see Refs. +# `M. Rossi et al, PRL (2016) `_, +# `V. Kapil et al, JCTC (2019) `_, +# `V. Kapil et al, PNAS (2022) `_). +# +# +# The central idea is to reversibly change the potential from harmonic to anharmonic +# by defining a :math:`\lambda`-dependent Hamiltonian +# +# .. math:: +# \hat{H}(\lambda) = \hat{T} + \lambda +# \hat{V}^{\text{harm}} + (1 - \lambda) \hat{V} +# +# The the anharmonic free energy is calculated as the reversible work done +# along the fictitious path in :math:`\lambda`-space +# +# .. math:: +# F = F^{\text{harm}} + \left< \hat{V} - +# \hat{V}^{\text{harm}} \right>_{\lambda} +# +# +# where :math:`\left< \hat{O} \right>_{\lambda}` +# is the path-integral estimator for a positon dependent operator +# for :math:`\hat{H}(\lambda)`. + + + From 13aeefcce7765f97096819a8ed7949863e3e8818 Mon Sep 17 00:00:00 2001 From: DavideTisi Date: Wed, 13 Nov 2024 17:42:04 +0100 Subject: [PATCH 4/8] add folders --- examples/free-energy/geop/init.xyz | 3 +++ examples/free-energy/geop/input.xml | 30 +++++++++++++++++++++++++++++ examples/free-energy/harm/input.xml | 27 ++++++++++++++++++++++++++ 3 files changed, 60 insertions(+) create mode 100644 examples/free-energy/geop/init.xyz create mode 100644 examples/free-energy/geop/input.xml create mode 100644 examples/free-energy/harm/input.xml diff --git a/examples/free-energy/geop/init.xyz b/examples/free-energy/geop/init.xyz new file mode 100644 index 00000000..18501ba9 --- /dev/null +++ b/examples/free-energy/geop/init.xyz @@ -0,0 +1,3 @@ +1 +# CELL(GENH): 100.0 0.0 0.0 0.0 100.0 0.0 0.0 0.0 100.0 positions{angstrom} cell{angstrom} +H 2.0 0.2 -0.5 diff --git a/examples/free-energy/geop/input.xml b/examples/free-energy/geop/input.xml new file mode 100644 index 00000000..68ed7233 --- /dev/null +++ b/examples/free-energy/geop/input.xml @@ -0,0 +1,30 @@ + + + [ step, potential ] + positions + + 1000 + + 32342 + + +
geop
+
+ + + geop/init.xyz + + + + + + + + 1e-5 + 1e-5 + 1e-5 + + + + +
diff --git a/examples/free-energy/harm/input.xml b/examples/free-energy/harm/input.xml new file mode 100644 index 00000000..a44e04d7 --- /dev/null +++ b/examples/free-energy/harm/input.xml @@ -0,0 +1,27 @@ + + + [ step, potential ] + + 5000 + + 32342 + + +
vib
+
+ + + init_harm.xyz + + + + + + + 0.001 + phonons + none + + + +
From 105214a0886e461b053c4c7f7d6343802f69128b Mon Sep 17 00:00:00 2001 From: DavideTisi Date: Wed, 13 Nov 2024 18:15:59 +0100 Subject: [PATCH 5/8] last-part --- examples/free-energy/free-energy.py | 60 ++++++++++++++++++++++++++++- 1 file changed, 59 insertions(+), 1 deletion(-) diff --git a/examples/free-energy/free-energy.py b/examples/free-energy/free-energy.py index 3368f911..96b30941 100644 --- a/examples/free-energy/free-energy.py +++ b/examples/free-energy/free-energy.py @@ -263,7 +263,7 @@ def PES(x, y , z): # The initial configuration for this calculation should correspond to an # opitimized position. You can obtain this from the last frame of the geop trajectory. -ase.io.write('init_harm.xyz',geop_traj,format='extxyz') +ase.io.write('init_harm.xyz',geop_traj[-1],format='extxyz') # %% # The `bash` command for this would be @@ -405,5 +405,63 @@ def quantum_harmonic_free_energy(Ws, T): # is the path-integral estimator for a positon dependent operator # for :math:`\hat{H}(\lambda)`. +# %% +# +# Step 3: Harmonic to anharmonic thermodynamic integration +# -------------------------------------------------------- +# +# A full quantum thermodynamic integration calculation requires +# knowledge of the harmonic reference. Luckily we have just performed these +# calculations! +# + +# %% +# Classical Statistical Mechanics +# ------------------------------- +# +# Let's first compute the anharmonic free energy difference within the classical approximation. +# +# To create the input file for I-PI we need to defines a "mixed" +# :math:`\lambda`-dependent Hamiltonian. Let's see the new most important parts. +# +# This i-PI calculation includes two "forcefield classes" +# +# .. code-block:: xml +# +# defines the anharmonic PES <--> +# +#
f0
+# 1e-3 +#
+# +# a standard socket +# +# and +# +# .. code-block:: xml +# +# defines the harmonic PES <--> +# +# HESSIAN-FILE +# X-REF-FILE relative path to a file containing the optimized positon vector <--> +# V-REF the value of the PES at its local minimum <--> +# +# +# an intrinsic harmonic forcefield that builds the harmonic potential. +# This requires :math:`q_0`, :math:`V(q_0)` and the full Hessian. +# `HESSIAN-FILE` is `harm.phonons.hess` which is the file containing the +# full hessian. +# X-REF-FILE is a file with the optimized positon vector +# + +with open('ref.data','w') as xref: + for pos in geop_traj[-1].positions: + xref.write(f'{pos[0]} {pos[1]} {pos[2]} \n') + +# V-REF can be obtained from the potential energy in `harm.out` + +V-ref = np.readtxt('harm.out') +print(V-ref) + From a09d177d021d0186fef2c488a22b518db7629be5 Mon Sep 17 00:00:00 2001 From: DavideTisi Date: Tue, 10 Dec 2024 18:08:48 +0100 Subject: [PATCH 6/8] finish and works --- examples/free-energy/cti/init.xyz | 3 + examples/free-energy/environment.yml | 2 +- examples/free-energy/free-energy.py | 644 +++++++++++++++++++++------ examples/free-energy/qti/init.xyz | 3 + 4 files changed, 526 insertions(+), 126 deletions(-) create mode 100644 examples/free-energy/cti/init.xyz create mode 100644 examples/free-energy/qti/init.xyz diff --git a/examples/free-energy/cti/init.xyz b/examples/free-energy/cti/init.xyz new file mode 100644 index 00000000..8032e3da --- /dev/null +++ b/examples/free-energy/cti/init.xyz @@ -0,0 +1,3 @@ +1 +# CELL(abcABC): 188.97261 188.97261 188.97261 90.00000 90.00000 90.00000 Step: 13 Bead: 0 positions{atomic_unit} cell{atomic_unit} + H 1.99641e+00 -6.18337e-10 1.54584e-09 diff --git a/examples/free-energy/environment.yml b/examples/free-energy/environment.yml index 35f747cc..c18b1d79 100644 --- a/examples/free-energy/environment.yml +++ b/examples/free-energy/environment.yml @@ -8,9 +8,9 @@ dependencies: - make - git - plumed - - py-plumed - pip: - ase==3.22.1 + - pyfftw - chemiscope - git+https://github.com/i-pi/i-pi.git@main#egg=ipi - matplotlib diff --git a/examples/free-energy/free-energy.py b/examples/free-energy/free-energy.py index 96b30941..69535352 100644 --- a/examples/free-energy/free-energy.py +++ b/examples/free-energy/free-energy.py @@ -17,13 +17,12 @@ import subprocess import time -import ipi import ase.io import chemiscope +import ipi import ipi.utils.parsing as pimdmooc -import numpy as np import matplotlib.pyplot as plt - +import numpy as np # %% @@ -35,18 +34,18 @@ # Ref. `Y. Litman et al., JCP (2022) # `_ # Its potential energy surface (PES) is described by the function -# +# # .. math:: # # V = A x^2 + B x^4 + \frac{1}{2} m \omega^2 y^2 + \frac{1}{2} m \omega^2 z^2 -# +# # with: -# +# # .. math:: -# +# # \begin{align} -# m &= 1837.107~\text{a.u.}\\ -# \omega &= 3800 ~\text{cm}^{-1} = 0.017314074~\text{a.u.}\\ +# m &= 1837.107~\text{a.u.}\\ +# \omega &= 3800 ~\text{cm}^{-1} = 0.017314074~\text{a.u.}\\ # A &= -0.00476705894242374~\text{a.u.}\\ # B &= 0.000598024968321866~\text{a.u.}\\ # \end{align} @@ -54,24 +53,26 @@ # Let's define a function to visualize the PES! # -def PES(x, y , z): + +def PES(x, y, z): """ PES from Ref. `Y. Litman et al., JCP (2022)` """ - + A = -0.00476705894242374 - B = 0.000598024968321866 + B = 0.000598024968321866 k = 1837.107 * 0.017314074**2 - - return A * x**2 + B * x**4 + k * y**2 / 2 + k * z**2 / 2 + + return A * x**2 + B * x**4 + k * y**2 / 2 + k * z**2 / 2 + # %% # The PES, in three dimensions, can be drawn with xy contours -# (each contour corresponds to kB T with T = 300 K), for various z values. +# (each contour corresponds to kB T with T = 300 K), for various z values. # -x = np.linspace(-3,3,21) -y = np.linspace(-0.5,0.5,21) +x = np.linspace(-3, 3, 21) +y = np.linspace(-0.5, 0.5, 21) X, Y = np.meshgrid(x, y) Z = PES(X, Y, 0) @@ -79,9 +80,9 @@ def PES(x, y , z): contour_levels = [np.min(Z) + 0.00095004347 * i for i in range(12)] -plt.title(r'$V(x,y,0)$') -plt.xlabel(r'$x$ [a.u.]') -plt.ylabel(r'$y$ [a.u.]') +plt.title(r"$V(x,y,0)$") +plt.xlabel(r"$x$ [a.u.]") +plt.ylabel(r"$y$ [a.u.]") plt.contour(X, Y, Z, levels=contour_levels) plt.show() @@ -92,7 +93,7 @@ def PES(x, y , z): # if delocalization of the system to its other minimum is # a rare event with respect to the time scale of # the system's vibrations? -# +# # 2. Feel free to plot it for various z values. # Does the plot change? What does it tell you # about the coupling between the modes? @@ -109,7 +110,7 @@ def PES(x, y , z): # The harmonic approximation to the PES is essentially # a truncated Taylor series expansion to second # order around one of its minima. -# :math:`V^{\text{harm}} = V(q_0) + \frac{2}{2} \left.\frac{\partial^2 V}{\partial q^2}\right|_{q_0} (q - q_0)^2` +# :math:`V^{\text{harm}} = V(q_0) + \frac{2}{2} \left.\frac{\partial^2 V}{\partial q^2}\right|_{q_0} (q - q_0)^2` # where :math:`q = (x,y,z)` # is a position vector and :math:`q_0 = \text{arg min}_{q} V` is # the position where the PES has a local minimum. @@ -121,7 +122,7 @@ def PES(x, y , z): # %% # Step 1: fixed cell geometry optimization # ---------------------------------------- -# +# # To find :math:`q_0` we will use the fixed-cell geometry # optimization feature of i-PI! The inputs are # into the `geop` directory. @@ -129,7 +130,7 @@ def PES(x, y , z): # You will find the i-PI input file. Have a look at the # `input.xml` file and see if you can understand its various parts. # -# The snippet that implements the geometry optimization feature is +# The snippet that implements the geometry optimization feature is # # .. code-block:: xml # @@ -151,7 +152,7 @@ def PES(x, y , z): # here we use the robust # `BFGS `_ # method. The tolerances set thershold values for changes in the energy, -# positions and forces, that are sufficient to deem an optimization converged. +# positions and forces, that are sufficient to deem an optimization converged. # # %% @@ -164,31 +165,33 @@ def PES(x, y , z): ipi.install_driver() # %% # To perform a fixed-cell geomerty optimization -# the bash script command should look like: -# +# the bash script command should look like: +# # .. code-block:: bash # # i-pi geop/input.xml > log.i-pi $ # sleep(5) -# i-pi-driver -u -h geop -m doublewell_1D & -# +# i-pi-driver -u -h geop -m doublewell_1D & +# # The same can be achieved from Python using `subprocess.Popen` +ipi_process = None +if not os.path.exists("geop.out"): + ipi_process = subprocess.Popen(["i-pi", "geop/input.xml"]) + time.sleep(5) # wait for i-PI to start + driver_process = subprocess.Popen( + ["i-pi-driver", "-u", "-h", "geop", "-m", "doublewell_1D"] + ) -ipi_process = subprocess.Popen(["i-pi", "geop/input.xml"]) -time.sleep(5) # wait for i-PI to start -driver_process =subprocess.Popen( - ["i-pi-driver", "-u", "-h", "geop", "-m", "doublewell_1D"] - ) - # %% # If you run this in a notebook, you can go ahead and start loading # output files *before* i-PI and lammps have finished running, by # skipping this cell -ipi_process.wait() -driver_process.wait() - +if ipi_process is not None: + ipi_process.wait() + driver_process.wait() + # %% # # The number of steps taken for an optimization calculation depends on @@ -200,26 +203,22 @@ def PES(x, y , z): # You can analyze your optimization calculation by plotting # the potential energy vs steps and confirm if the potential # energy has indeed converged to the set threshold! -# -# The final frame of the `geop.pos_0.xyz` file gives -# with chemiscope we can wisualize the minimzation +# +# The final frame of the `geop.pos_0.xyz` file gives +# with chemiscope we can wisualize the minimzation # trajectory and its energies. # -geop_out,_geop = ipi.read_output('geop.out') +geop_out, _geop = ipi.read_output("geop.out") geop_traj = ipi.read_trajectory("geop.pos_0.xyz") chemiscope.show( frames=geop_traj, properties={ - "steps": { "values" : np.arange(len(geop_traj)), - "target" : "structure"}, - "U":{"values": geop_out['potential'], - "target" : "structure"}, - }, - settings=chemiscope.quick_settings( - x="steps", y="U", trajectory=True - ), + "steps": {"values": np.arange(len(geop_traj)), "target": "structure"}, + "U": {"values": geop_out["potential"], "target": "structure"}, + }, + settings=chemiscope.quick_settings(x="steps", y="U", trajectory=True), mode="structure", ) @@ -227,10 +226,10 @@ def PES(x, y , z): # Step 2: harmonic calculation # ---------------------------- # -# To compute the system's Hessian we will use the vibrations feature of i-PI. +# To compute the system's Hessian we will use the vibrations feature of i-PI. # Go through the `input.xml` file. -# The snippet that implements the vibrations feature is -# +# The snippet that implements the vibrations feature is +# # .. code-block:: xml # # @@ -261,69 +260,79 @@ def PES(x, y , z): # %% # The initial configuration for this calculation should correspond to an -# opitimized position. You can obtain this from the last frame of the geop trajectory. +# opitimized position. You can obtain this from the last frame of the geop trajectory. -ase.io.write('init_harm.xyz',geop_traj[-1],format='extxyz') +ase.io.write("init_harm.xyz", geop_traj[-1], format="extxyz") # %% # The `bash` command for this would be -# +# # .. code-block:: bash # # i-pi harm/input.xml > log.i-pi $ # sleep(5) -# i-pi-driver -u -h vib -m doublewell_1D & -# +# i-pi-driver -u -h vib -m doublewell_1D & +# # Again we will use `subprocess.Popen` -ipi_process = subprocess.Popen(["i-pi", "harm/input.xml"]) -time.sleep(5) # wait for i-PI to start -driver_process =subprocess.Popen( - ["i-pi-driver", "-u", "-h", "vib", "-m", "doublewell_1D"] - ) +ipi_process = None +if not os.path.exists("harm.out"): + ipi_process = subprocess.Popen(["i-pi", "harm/input.xml"]) + time.sleep(5) # wait for i-PI to start + driver_process = subprocess.Popen( + ["i-pi-driver", "-u", "-h", "vib", "-m", "doublewell_1D"] + ) # %% # If you run this in a notebook, you can go ahead and start loading # output files *before* i-PI and lammps have finished running, by # skipping this cell -ipi_process.wait() -driver_process.wait() +if ipi_process is not None: + ipi_process.wait() + driver_process.wait() # %% -# The Hessian can be recovered from the `harm.phonons.hess` file. +# The Hessian can be recovered from the `harm.phonons.hess` file. # You can use the snippet below to plot the harmonic approximation # to the PES # -def PES_harm(x,y,z): + +def PES_harm(x, y, z): """ - Harmonic approximation to the PES from Ref. `Y. Litman et al., JCP (2022)` around + Harmonic approximation to the PES from Ref. `Y. Litman et al., JCP (2022)` around a local minimum. Note this function is only valid for the example! """ - - return V0 + hess[0,0] * (x - q0[0])**2 / 2 + hess[1,1] * (y - q0[1])**2 / 2 + hess[2,2] * (z - q0[2])**2 / 2 -hess = np.loadtxt('harm.phonons.hess', comments='#') -q0 = ipi.read_trajectory('init_harm.xyz')[0].positions[0] / 0.529177 -V0 = np.loadtxt('harm.out', ndmin=2)[0,1] + return ( + V0 + + hess[0, 0] * (x - q0[0]) ** 2 / 2 + + hess[1, 1] * (y - q0[1]) ** 2 / 2 + + hess[2, 2] * (z - q0[2]) ** 2 / 2 + ) + -x = np.linspace(-3,3,21) -y = np.linspace(-0.5,0.5,21) +hess = np.loadtxt("harm.phonons.hess", comments="#") +q0 = ipi.read_trajectory("init_harm.xyz")[0].positions[0] / 0.529177 +V0 = np.loadtxt("harm.out", ndmin=2)[0, 1] + +x = np.linspace(-3, 3, 21) +y = np.linspace(-0.5, 0.5, 21) X, Y = np.meshgrid(x, y) contour_levels = [np.min(Z) + 0.00095004347 * i for i in range(12)] -plt.title(r'$V(x,y,0)$') -plt.xlabel(r'$x$ [a.u.]') -plt.ylabel(r'$y$ [a.u.]') +plt.title(r"$V(x,y,0)$") +plt.xlabel(r"$x$ [a.u.]") +plt.ylabel(r"$y$ [a.u.]") plt.contour(X, Y, PES(X, Y, 0), levels=contour_levels) plt.show() -plt.title(r'$V^{\mathrm{harm}}(x,y,0)$') -plt.xlabel(r'$x$ [a.u.]') -plt.ylabel(r'$y$ [a.u.]') +plt.title(r"$V^{\mathrm{harm}}(x,y,0)$") +plt.xlabel(r"$x$ [a.u.]") +plt.ylabel(r"$y$ [a.u.]") plt.contour(X, Y, PES_harm(X, Y, 0), levels=contour_levels) plt.show() @@ -332,45 +341,56 @@ def PES_harm(x,y,z): # from the dynamical matrix (mass scaled hessian)! # -W2s = np.loadtxt('harm.phonons.eigval') -print ('Harmonic Frequencies') +W2s = np.loadtxt("harm.phonons.eigval") +print("Harmonic Frequencies") for w2 in W2s: - print('%10.5f cm^-1'% (w2**0.5 * 219474)) + print("%10.5f cm^-1" % (w2**0.5 * 219474)) -# %% +# %% # These frequencies can be used to calculate the quantum harmonic # free energy of the system -- an approxiamtion to its true free energy! # + def quantum_harmonic_free_energy(Ws, T): """ - Receives a list of frequencies in atomic units and the temperature + Receives a list of frequencies in atomic units and the temperature in Kelvin. Returns the system's harmonic free energy. """ - + hbar = 1 kB = 3.1668116e-06 - - return V0 + -kB * T * np.log(1 - np.exp(-hbar * Ws / (kB * T))).sum() -print ('Quantum Harmonic free energy: %15.8f [a.u.]'% (quantum_harmonic_free_energy(W2s**0.5, 300))) -print ('Quantum Harmonic free energy: %15.8f [eV]'% (quantum_harmonic_free_energy(W2s**0.5, 300) * 27.211386)) -print ('Quantum Harmonic free energy: %15.8f [kJ/mol]' % (quantum_harmonic_free_energy(W2s**0.5, 300) * 2625.4996)) + return V0 + -kB * T * np.log(1 - np.exp(-hbar * Ws / (kB * T))).sum() + + +print( + "Quantum Harmonic free energy: %15.8f [a.u.]" + % (quantum_harmonic_free_energy(W2s**0.5, 300)) +) +print( + "Quantum Harmonic free energy: %15.8f [eV]" + % (quantum_harmonic_free_energy(W2s**0.5, 300) * 27.211386) +) +print( + "Quantum Harmonic free energy: %15.8f [kJ/mol]" + % (quantum_harmonic_free_energy(W2s**0.5, 300) * 2625.4996) +) # %% # # The exact free energy for the system when localized in one of -# the wells is still around 0.65 kJ/mol off w.r.t the harmonic limit. +# the wells is still around 0.65 kJ/mol off w.r.t the harmonic limit. # F = -7.53132797e-05 + quantum_harmonic_free_energy(W2s**0.5, 300) -print ('Exact Quantum free energy: %15.8f [a.u.]'% (F)) -print ('Exact Quantum free energy: %15.8f [eV]'% (F * 27.211386)) -print ('Exact Quantum free energy: %15.8f [kJ/mol]' % (F * 2625.4996)) +print("Exact Quantum free energy: %15.8f [a.u.]" % (F)) +print("Exact Quantum free energy: %15.8f [eV]" % (F * 27.211386)) +print("Exact Quantum free energy: %15.8f [kJ/mol]" % (F * 2625.4996)) # %% -# +# # Harmonic to anharmonic # ---------------------- # @@ -379,15 +399,15 @@ def quantum_harmonic_free_energy(Ws, T): # Equation by approximating the anharmonic component of the PES, yielding an amharmonic # free energy. While highly effective for low-dimensional or mildly anharmonic systems, # the method of resort for *numerically-exact amharmonic free energies* of solid and clusters -# is the thermodynamic integration method combined with the path-integral method +# is the thermodynamic integration method combined with the path-integral method # ( for applications see Refs. # `M. Rossi et al, PRL (2016) `_, # `V. Kapil et al, JCTC (2019) `_, # `V. Kapil et al, PNAS (2022) `_). -# +# # # The central idea is to reversibly change the potential from harmonic to anharmonic -# by defining a :math:`\lambda`-dependent Hamiltonian +# by defining a :math:`\lambda`-dependent Hamiltonian # # .. math:: # \hat{H}(\lambda) = \hat{T} + \lambda @@ -401,8 +421,8 @@ def quantum_harmonic_free_energy(Ws, T): # \hat{V}^{\text{harm}} \right>_{\lambda} # # -# where :math:`\left< \hat{O} \right>_{\lambda}` -# is the path-integral estimator for a positon dependent operator +# where :math:`\left< \hat{O} \right>_{\lambda}` +# is the path-integral estimator for a positon dependent operator # for :math:`\hat{H}(\lambda)`. # %% @@ -412,7 +432,7 @@ def quantum_harmonic_free_energy(Ws, T): # # A full quantum thermodynamic integration calculation requires # knowledge of the harmonic reference. Luckily we have just performed these -# calculations! +# calculations! # # %% @@ -420,48 +440,422 @@ def quantum_harmonic_free_energy(Ws, T): # ------------------------------- # # Let's first compute the anharmonic free energy difference within the classical approximation. -# +# # To create the input file for I-PI we need to defines a "mixed" -# :math:`\lambda`-dependent Hamiltonian. Let's see the new most important parts. +# :math:`\lambda`-dependent Hamiltonian. Let's see the new most important parts. # -# This i-PI calculation includes two "forcefield classes" +# This i-PI calculation includes two "forcefield classes" # # .. code-block:: xml -# +# # defines the anharmonic PES <--> # #
f0
# 1e-3 #
-# -# a standard socket -# -# and -# +# +# a standard socket +# +# and +# # .. code-block:: xml # # defines the harmonic PES <--> # -# HESSIAN-FILE -# X-REF-FILE relative path to a file containing the optimized positon vector <--> -# V-REF the value of the PES at its local minimum <--> +# HESSIAN_FILE +# X_REF_FILE relative path to a file containing the optimized positon vector <--> +# V_REF the value of the PES at its local minimum <--> # -# +# # an intrinsic harmonic forcefield that builds the harmonic potential. -# This requires :math:`q_0`, :math:`V(q_0)` and the full Hessian. -# `HESSIAN-FILE` is `harm.phonons.hess` which is the file containing the +# This requires :math:`q_0`, :math:`V(q_0)` and the full Hessian. +# `HESSIAN_FILE` is `harm.phonons.hess` which is the file containing the # full hessian. -# X-REF-FILE is a file with the optimized positon vector -# +# X_REF_FILE is a file with the optimized positon vector +# + -with open('ref.data','w') as xref: +HESSIAN_FILE = "harm.phonons.hess" +X_REF_FILE = "ref.data" +with open(X_REF_FILE, "w") as xref: for pos in geop_traj[-1].positions: - xref.write(f'{pos[0]} {pos[1]} {pos[2]} \n') + xref.write(f"{pos[0]} {pos[1]} {pos[2]} \n") + +# %% +# V_REF can be obtained from the potential energy in `harm.out` + +V_REF = np.loadtxt("harm.out")[1] +print(V_REF) + +# %% +# To model a Hamiltonian with a linear combination of the harmonic and +# the anharmonic potential you can define the weights for the force +# components as +# +# .. code-block:: xml +# +# +# set this to lambda <--> +# set this to 1 - lambda <--> +# +# +# You can print out the harmonic and the anharmonic +# components as a in the output class +# +# .. code-block:: xml +# +# +# [ pot_component_raw(0), pot_component_raw(1) ] +# +# +# A typical TI calculation requires multiple simulations, +# one for each lambda and a postprocessing step to integrate the free +# energy difference. In this example, we use six linearly-spaced points i.e. +# :math:`\lambda\in\left[0, 0.2, 0.4, 0.6, 0.8, 1.0\right]`, +# and create a set of files for each calculation. + +# %% +# Let's generate the input files for the TI calculations + +for idx, i in enumerate(["0.0", "0.2", "0.4", "0.6", "0.8", "1.0"]): + with open(f"cti/input_{i}.xml", "w") as f: + strfile = """ + + [ step, time{{picosecond}}, conserved, temperature{{kelvin}}, kinetic_cv, potential, pressure_cv, volume, ensemble_temperature ] + [ pot_component_raw(0), pot_component_raw(1) ] + positions + x_centroid + + + 10000 + 31415 + +
f{idx}
+ 1e-3 +
+ + {HESSIAN_FILE} + {X_REF_FILE} + {V_REF} + + + + ./cti/init.xyz + 300 + + + + + + + False + + 1.00 + + 100 + + + + + 300 + + +
+""".format( + HESSIAN_FILE=HESSIAN_FILE, + X_REF_FILE=X_REF_FILE, + V_REF=V_REF, + i=i, + idx=idx, + im1=1 - float(i), + ) + f.write(strfile) + +# %% +# You can run i-PI simulataneous in these directories, the bash command would look like: +# +# .. code-block:: bash +# +# for x in 0.0 0.2 0.4 0.6 0.8 1.0 ; do +# cd ${x} +# i-pi cti/input_${x}.xml > log${x}.i-pi & +# cd .. +# done +# +# wait 5 +# +# for x in {0..10..2}; do +# i-pi-driver -u -h f${x} -m doublewell_1D & +# done +# + +for idx, i in enumerate(["0.0", "0.2", "0.4", "0.6", "0.8", "1.0"]): + ipi_process = None + if not os.path.exists(f"cti_{i}.out"): + ipi_process = subprocess.Popen(["i-pi", f"cti/input_{i}.xml"]) + time.sleep(5) # wait for i-PI to start + driver_process = subprocess.Popen( + ["i-pi-driver", "-u", "-h", f"f{idx}", "-m", "doublewell_1D"] + ) + # in a jupiter notebook comments the next 3 lines to be able to + # load the outputs before the run ends + if ipi_process is not None: + ipi_process.wait() + driver_process.wait() + +# %% +# +# When the calculations have finished, +# you can use the following snippet to analyze the +# mean force along the path and estimat its integral! + +du_list = [] +duerr_list = [] + +dir_list = ["0.0", "0.2", "0.4", "0.6", "0.8", "1.0"] +l_list = [float(l) for l in dir_list] + +for i in dir_list: + + filename = f"cti_{i}.pots" + data, _data = ipi.read_output(filename) + + du = data["pot_component_raw(1)"] - data["pot_component_raw(0)"] + du_list.append(du.mean()) + duerr_list.append(du.std() / len(du) ** 0.5) + + +du_list = np.asarray(du_list) +duerr_list = np.asarray(duerr_list) + +plt.plot(l_list, (du_list) * 2625.4996, color="blue") +plt.fill_between( + l_list, + y1=(du_list - duerr_list) * 2625.4996, + y2=(du_list + duerr_list) * 2625.4996, + color="blue", + alpha=0.2, +) +plt.title("Classical thermodynamic integration") +plt.xlabel(r"$\lambda$") +plt.ylabel(r"$\left_{\lambda}$ [kJ/mol]") +plt.show() -# V-REF can be obtained from the potential energy in `harm.out` -V-ref = np.readtxt('harm.out') -print(V-ref) +# %% +# Since we are working within classical stat mech, +# we should use the classical harmonic reference to estimate +# the classical anharmonic free energy. + + +def classical_harmonic_free_energy(Ws, T): + """ + Receives a list of frequencies in atomic units and + the temperature in Kelvin. Returns the system's harmonic free energy. + """ + + hbar = 1 + kB = 3.1668116e-06 + + return V0 + kB * T * np.log(hbar * Ws / (kB * T)).sum() +df, dferr = np.trapz(x=l_list, y=du_list), np.trapz(x=l_list, y=duerr_list**2) ** 0.5 + +F = classical_harmonic_free_energy(W2s**0.5, 300) + +print("Classical harmonic free energy: %15.8f [a.u.]" % (F)) +print("Classical harmonic free energy: %15.8f [eV]" % (F * 27.211386)) +print("Classical harmonic free energy: %15.8f [kJ/mol]" % (F * 2625.4996)) +print("") + +F = classical_harmonic_free_energy(W2s**0.5, 300) + df +Ferr = dferr + + +print("Classical anharmonic free energy: %15.8f +/- %15.8f [a.u.]" % (F, Ferr)) +print( + "Classical anharmonic free energy: %15.8f +/- %15.8f [eV]" + % (F * 27.211386, Ferr * 27.211386) +) +print( + "Classical anharmonic free energy: %15.8f +/- %15.8f [kJ/mol]" + % (F * 2625.4996, Ferr * 2625.4996) +) +print("") +F = -7.53132797e-05 + quantum_harmonic_free_energy(W2s**0.5, 300) + +print("Exact free energy: %15.8f [a.u.]" % (F)) +print("Exact free energy: %15.8f [eV]" % (F * 27.211386)) +print("Exact free energy: %15.8f [kJ/mol]" % (F * 2625.4996)) + + +# %% +# Quantum Statistical Mechanics +# ----------------------------- +# +# The quantum anharmonic free energy can be calculated using the path-integral +# method. The main difference in the input file is the number of replicas! +# Let's construct the input file: + +for idx, i in enumerate(["0.0", "0.2", "0.4", "0.6", "0.8", "1.0"]): + with open(f"qti/input_{i}.xml", "w") as f: + strfile = """ + + [ step, time{{picosecond}}, conserved, temperature{{kelvin}}, kinetic_cv, potential, pressure_cv, volume, ensemble_temperature ] + [ pot_component_raw(0), pot_component_raw(1) ] + positions + x_centroid + + + 10000 + 31415 + +
f{idx}
+ 1e-3 +
+ + {HESSIAN_FILE} + {X_REF_FILE} + {V_REF} + + + + ./qti/init.xyz + 300 + + + + + + + False + + 1.00 + + 100 + + + + + 300 + + +
+""".format( + HESSIAN_FILE=HESSIAN_FILE, + X_REF_FILE=X_REF_FILE, + V_REF=V_REF, + i=i, + idx=idx, + im1=1 - float(i), + ) + f.write(strfile) + + +# %% +# You can run i-PI simulataneous. + +for idx, i in enumerate(["0.0", "0.2", "0.4", "0.6", "0.8", "1.0"]): + ipi_process = None + if not os.path.exists(f"qti_{i}.out"): + ipi_process = subprocess.Popen(["i-pi", f"qti/input_{i}.xml"]) + time.sleep(5) # wait for i-PI to start + driver_process = [ + subprocess.Popen( + ["i-pi-driver", "-u", "-h", f"f{idx}", "-m", "doublewell_1D"] + ) + for i in range(32) + ] + # in a jupiter notebook comments the next 3 lines to be able to + # load the outputs before the run ends + if ipi_process is not None: + ipi_process.wait() + for i in range(32): + driver_process[i].wait() + +# %% +# The data analysys is done with the following snippets + +Q_du_list = [] +Q_duerr_list = [] + +Q_dir_list = ["0.0", "0.2", "0.4", "0.6", "0.8", "1.0"] +Q_l_list = [float(l) for l in Q_dir_list] + +for i in Q_dir_list: + filename = f"qti_{i}.pots" + data, _data = ipi.read_output(filename) + + du = data["pot_component_raw(1)"] - data["pot_component_raw(0)"] + Q_du_list.append(du.mean()) + Q_duerr_list.append(du.std() / len(du) ** 0.5) + + +Q_du_list = np.asarray(Q_du_list) +Q_duerr_list = np.asarray(Q_duerr_list) + +plt.plot( + Q_l_list, + (Q_du_list) * 2625.4996, + color="red", + label="Quantum thermodynamic integration", +) +plt.fill_between( + Q_l_list, + y1=(Q_du_list - Q_duerr_list) * 2625.4996, + y2=(Q_du_list + Q_duerr_list) * 2625.4996, + color="red", + alpha=0.2, +) +plt.plot( + l_list, + (du_list) * 2625.4996, + color="blue", + label="Classical thermodynamic integration", +) +plt.fill_between( + l_list, + y1=(du_list - duerr_list) * 2625.4996, + y2=(du_list + duerr_list) * 2625.4996, + color="blue", + alpha=0.2, +) +plt.legend() +plt.xlabel(r"$\lambda$") +plt.ylabel(r"$\left_{\lambda}$ [kJ/mol]") + +# %% +# Then show the free energy + +df, dferr = ( + np.trapz(x=Q_l_list, y=Q_du_list), + np.trapz(x=Q_l_list, y=Q_duerr_list**2) ** 0.5, +) + +F = quantum_harmonic_free_energy(W2s**0.5, 300) + +print("Quantum harmonic free energy: %15.8f [a.u.]" % (F)) +print("Quantum harmonic free energy: %15.8f [eV]" % (F * 27.211386)) +print("Quantum harmonic free energy: %15.8f [kJ/mol]" % (F * 2625.4996)) +print("") + +F = quantum_harmonic_free_energy(W2s**0.5, 300) + df +Ferr = dferr + + +print("Quantum anharmonic free energy: %15.8f +/- %15.8f [a.u.]" % (F, Ferr)) +print( + "Quantum anharmonic free energy: %15.8f +/- %15.8f [eV]" + % (F * 27.211386, Ferr * 27.211386) +) +print( + "Quantum anharmonic free energy: %15.8f +/- %15.8f [kJ/mol]" + % (F * 2625.4996, Ferr * 2625.4996) +) +print("") +F = -7.53132797e-05 + quantum_harmonic_free_energy(W2s**0.5, 300) +print("Exact free energy: %15.8f [a.u.]" % (F)) +print("Exact free energy: %15.8f [eV]" % (F * 27.211386)) +print("Exact free energy: %15.8f [kJ/mol]" % (F * 2625.4996)) diff --git a/examples/free-energy/qti/init.xyz b/examples/free-energy/qti/init.xyz new file mode 100644 index 00000000..8032e3da --- /dev/null +++ b/examples/free-energy/qti/init.xyz @@ -0,0 +1,3 @@ +1 +# CELL(abcABC): 188.97261 188.97261 188.97261 90.00000 90.00000 90.00000 Step: 13 Bead: 0 positions{atomic_unit} cell{atomic_unit} + H 1.99641e+00 -6.18337e-10 1.54584e-09 From 0c492093fe5de3c7776a744a601f94d197f77fa9 Mon Sep 17 00:00:00 2001 From: DavideTisi Date: Tue, 10 Dec 2024 18:35:59 +0100 Subject: [PATCH 7/8] linter --- examples/free-energy/free-energy.py | 85 ++++++++++++++++++----------- 1 file changed, 52 insertions(+), 33 deletions(-) diff --git a/examples/free-energy/free-energy.py b/examples/free-energy/free-energy.py index 69535352..763b4f7e 100644 --- a/examples/free-energy/free-energy.py +++ b/examples/free-energy/free-energy.py @@ -20,7 +20,6 @@ import ase.io import chemiscope import ipi -import ipi.utils.parsing as pimdmooc import matplotlib.pyplot as plt import numpy as np @@ -110,7 +109,8 @@ def PES(x, y, z): # The harmonic approximation to the PES is essentially # a truncated Taylor series expansion to second # order around one of its minima. -# :math:`V^{\text{harm}} = V(q_0) + \frac{2}{2} \left.\frac{\partial^2 V}{\partial q^2}\right|_{q_0} (q - q_0)^2` +# :math:`V^{\text{harm}} = V(q_0) + +# \frac{1}{2} \left.\frac{\partial^2 V}{\partial q^2}\right|_{q_0} (q - q_0)^2` # where :math:`q = (x,y,z)` # is a position vector and :math:`q_0 = \text{arg min}_{q} V` is # the position where the PES has a local minimum. @@ -150,7 +150,7 @@ def PES(x, y, z): # simply move towards a local minimum of the PES. There are # many algorithms for locally optimizing high-dimensional functions; # here we use the robust -# `BFGS `_ +# `BFGS` (Broyden-Fletcher-Goldfarb-Shanno) quasi-Newton # method. The tolerances set thershold values for changes in the energy, # positions and forces, that are sufficient to deem an optimization converged. # @@ -252,8 +252,10 @@ def PES(x, y, z): # - \epsilon} \right) # # At every step instead of performing "dynamics", we will displace a degree of -# freedom along :math:`\pm \epsilon` and estimate one row of the Hessian. `pos_shift` sets -# the value of :math:`\epsilon` while `asr` zeros out the blocks of the Hessian due to continuous +# freedom along :math:`\pm \epsilon` and estimate one row of the Hessian. +# `pos_shift` sets +# the value of :math:`\epsilon` while `asr` zeros out the blocks +# of the Hessian due to continuous # symmetries (translations or rotations for solids or clusters). In this example, # we set this option to `none` as our system doesn't possess any continuous symmetries. # @@ -396,9 +398,11 @@ def quantum_harmonic_free_energy(Ws, T): # # Calculating free energies beyond the harmonic approximation is non-trivial. # There exist a familty of methods that can solve the vibrational Schroedinger -# Equation by approximating the anharmonic component of the PES, yielding an amharmonic +# Equation by approximating the anharmonic component of +# the PES, yielding an amharmonic # free energy. While highly effective for low-dimensional or mildly anharmonic systems, -# the method of resort for *numerically-exact amharmonic free energies* of solid and clusters +# the method of resort for *numerically-exact amharmonicfree energies* +# of solid and clusters # is the thermodynamic integration method combined with the path-integral method # ( for applications see Refs. # `M. Rossi et al, PRL (2016) `_, @@ -439,7 +443,8 @@ def quantum_harmonic_free_energy(Ws, T): # Classical Statistical Mechanics # ------------------------------- # -# Let's first compute the anharmonic free energy difference within the classical approximation. +# Let's first compute the anharmonic free +# energy difference within the classical approximation. # # To create the input file for I-PI we need to defines a "mixed" # :math:`\lambda`-dependent Hamiltonian. Let's see the new most important parts. @@ -463,8 +468,12 @@ def quantum_harmonic_free_energy(Ws, T): # defines the harmonic PES <--> # # HESSIAN_FILE -# X_REF_FILE relative path to a file containing the optimized positon vector <--> -# V_REF the value of the PES at its local minimum <--> +# X_REF_FILE +# relative path to a file containing the optimized positon vector <--> +# +# V_REF +# the value of the PES at its local minimum <--> +# # # # an intrinsic harmonic forcefield that builds the harmonic potential. @@ -494,10 +503,10 @@ def quantum_harmonic_free_energy(Ws, T): # # .. code-block:: xml # -# -# set this to lambda <--> -# set this to 1 - lambda <--> -# +# +# set this to lambda <--> +# set this to 1 - lambda <--> +# # # You can print out the harmonic and the anharmonic # components as a in the output class @@ -521,9 +530,14 @@ def quantum_harmonic_free_energy(Ws, T): with open(f"cti/input_{i}.xml", "w") as f: strfile = """ - [ step, time{{picosecond}}, conserved, temperature{{kelvin}}, kinetic_cv, potential, pressure_cv, volume, ensemble_temperature ] - [ pot_component_raw(0), pot_component_raw(1) ] - positions + [ step, time{{picosecond}}, + conserved, temperature{{kelvin}}, kinetic_cv, potential, pressure_cv, + volume, ensemble_temperature ] + + [ pot_component_raw(0), pot_component_raw(1) ] + + positions + x_centroid @@ -534,13 +548,13 @@ def quantum_harmonic_free_energy(Ws, T): 1e-3 - {HESSIAN_FILE} - {X_REF_FILE} - {V_REF} + {HESSIAN_FILE} + {X_REF_FILE} + {V_REF} - ./cti/init.xyz + ./cti/init.xyz 300 @@ -548,7 +562,7 @@ def quantum_harmonic_free_energy(Ws, T): - False + False 1.00 @@ -584,7 +598,7 @@ def quantum_harmonic_free_energy(Ws, T): # # wait 5 # -# for x in {0..10..2}; do +# for x in {0..10}; do # i-pi-driver -u -h f${x} -m doublewell_1D & # done # @@ -613,7 +627,7 @@ def quantum_harmonic_free_energy(Ws, T): duerr_list = [] dir_list = ["0.0", "0.2", "0.4", "0.6", "0.8", "1.0"] -l_list = [float(l) for l in dir_list] +l_list = [float(lst) for lst in dir_list] for i in dir_list: @@ -702,9 +716,14 @@ def classical_harmonic_free_energy(Ws, T): with open(f"qti/input_{i}.xml", "w") as f: strfile = """ - [ step, time{{picosecond}}, conserved, temperature{{kelvin}}, kinetic_cv, potential, pressure_cv, volume, ensemble_temperature ] - [ pot_component_raw(0), pot_component_raw(1) ] - positions + [ step, time{{picosecond}}, + conserved, temperature{{kelvin}}, kinetic_cv, potential, + pressure_cv, volume, ensemble_temperature ] + + [ pot_component_raw(0), pot_component_raw(1) ] + + positions + x_centroid @@ -715,13 +734,13 @@ def classical_harmonic_free_energy(Ws, T): 1e-3 - {HESSIAN_FILE} - {X_REF_FILE} - {V_REF} + {HESSIAN_FILE} + {X_REF_FILE} + {V_REF} - ./qti/init.xyz + ./qti/init.xyz 300 @@ -729,7 +748,7 @@ def classical_harmonic_free_energy(Ws, T): - False + False 1.00 @@ -781,7 +800,7 @@ def classical_harmonic_free_energy(Ws, T): Q_duerr_list = [] Q_dir_list = ["0.0", "0.2", "0.4", "0.6", "0.8", "1.0"] -Q_l_list = [float(l) for l in Q_dir_list] +Q_l_list = [float(lst) for lst in Q_dir_list] for i in Q_dir_list: filename = f"qti_{i}.pots" From 4c0e5429ae1da4443af78852b5c16406126fedd5 Mon Sep 17 00:00:00 2001 From: DavideTisi Date: Tue, 10 Dec 2024 20:19:44 +0100 Subject: [PATCH 8/8] separate graph --- examples/free-energy/free-energy.py | 2 ++ 1 file changed, 2 insertions(+) diff --git a/examples/free-energy/free-energy.py b/examples/free-energy/free-energy.py index 763b4f7e..f804d2f1 100644 --- a/examples/free-energy/free-energy.py +++ b/examples/free-energy/free-energy.py @@ -332,6 +332,8 @@ def PES_harm(x, y, z): plt.contour(X, Y, PES(X, Y, 0), levels=contour_levels) plt.show() +# %% + plt.title(r"$V^{\mathrm{harm}}(x,y,0)$") plt.xlabel(r"$x$ [a.u.]") plt.ylabel(r"$y$ [a.u.]")