# flucq (c47b2)

Combined QM/MM Fluctuating Charge Potential for CHARMM

Ben Webb, ben@bellatrix.pcl.ox.ac.uk, and Paul Lyne

The fluctuating charge potential (FlucQ or FQ) is based on the method

developed by Rick, Stuart and Berne (Rick et. al., J. Chem. Phys. 101

(7) 1994 p6141) for molecular dynamics, and extended for hybrid QM/MM

simulations (Bryce et. al., Chem. Phys. Lett. 279 1997, p367). It is

designed primarily for computationally efficient (approx. 10% overhead)

modelling of solvent polarisation in hybrid QM/MM systems, and as such

is implemented for QUANTUM, CADPAC and GAMESS codes, although the

current implementation is easily extensible to any atom type and bond.

* Syntax | Syntax of the FLUCQ command

* Activation | Starting FlucQ from a CHARMM input file

* Charge solution | Solving for exact charges

* Reference energy | Setting the ``zero'' for FlucQ polarisation

* Caveats | Changes to be aware of; known limitations

* Using FlucQ with QM:: Necessary changes for use with CADPAC or GAMESS

* Examples | Simple uses of the FLUCQ command

* Implementation | Mathematical and computational details

Ben Webb, ben@bellatrix.pcl.ox.ac.uk, and Paul Lyne

The fluctuating charge potential (FlucQ or FQ) is based on the method

developed by Rick, Stuart and Berne (Rick et. al., J. Chem. Phys. 101

(7) 1994 p6141) for molecular dynamics, and extended for hybrid QM/MM

simulations (Bryce et. al., Chem. Phys. Lett. 279 1997, p367). It is

designed primarily for computationally efficient (approx. 10% overhead)

modelling of solvent polarisation in hybrid QM/MM systems, and as such

is implemented for QUANTUM, CADPAC and GAMESS codes, although the

current implementation is easily extensible to any atom type and bond.

* Syntax | Syntax of the FLUCQ command

* Activation | Starting FlucQ from a CHARMM input file

* Charge solution | Solving for exact charges

* Reference energy | Setting the ``zero'' for FlucQ polarisation

* Caveats | Changes to be aware of; known limitations

* Using FlucQ with QM:: Necessary changes for use with CADPAC or GAMESS

* Examples | Simple uses of the FLUCQ command

* Implementation | Mathematical and computational details

Top

[SYNTAX FLUCq]

FLUCq { ON init-spec (atom selection) }

{ OFF }

{ PRINt }

{ EXACt exac-spec }

{ REFErence { GAS exac-spec } }

{ { SOLVent exac-spec } }

{ { CURRent } }

{ { ENERgy real } }

DYNAmics ... thermo-spec

init-spec::= [GROUp] [NOFIxed]

exac-spec::= [TIMEstep real] [ZETA real]

[TQDEsired real] [PRINt]

thermo-spec::= [FQTEmp real] [FQUNit integer]

{ FQTCoupling real } ! weak coupling

{ FQMAss real nose-spec } ! Nose-Hoover

{ FQSCale integer } ! velocity scaling

nose-spec::= [FQTOlerance real] [FQITerations integer]

[SYNTAX FLUCq]

FLUCq { ON init-spec (atom selection) }

{ OFF }

{ PRINt }

{ EXACt exac-spec }

{ REFErence { GAS exac-spec } }

{ { SOLVent exac-spec } }

{ { CURRent } }

{ { ENERgy real } }

DYNAmics ... thermo-spec

init-spec::= [GROUp] [NOFIxed]

exac-spec::= [TIMEstep real] [ZETA real]

[TQDEsired real] [PRINt]

thermo-spec::= [FQTEmp real] [FQUNit integer]

{ FQTCoupling real } ! weak coupling

{ FQMAss real nose-spec } ! Nose-Hoover

{ FQSCale integer } ! velocity scaling

nose-spec::= [FQTOlerance real] [FQITerations integer]

Top

FlucQ code is enabled within CHARMM by means of the FLUCQ ON

command. Future energy calculations will then include an extra energy

term - FQPO, the FlucQ polarisation energy, while dynamics simulations

involve a new energy property - FQKI, the FlucQ charge kinetic energy.

Once FlucQ is active, the selected atoms are treated as extra degrees

of freedom, free to fluctuate under the charge forces in the system,

and, by assigning each atom type a fictional charge "mass", these

charges can be accelerated in a conventional dynamics simulation, in a

completely analogous way to the Cartesian degrees of freedom.

If atoms are selected by the FLUCQ command which cannot be modelled

(i.e. they are QM atoms, or have no FlucQ parameters defined for them)

they will be automatically removed from the selection.

The FlucQ polarisation energy, FQPO, is an intramolecular

interaction; in full electronegativity equalisation, every atom

interacts through space, by means of a modified Coulomb-type

interaction, with every other atom in the molecule. In this

implementation, the only interactions calculated are those along

defined CHARMM bonds (even those with zero force constants).

[GROUp] conserves charge within groups, rather than the default

behaviour of conserving charge within residues; this prohibits charge

transfer between groups. Note that the FlucQ model makes no restriction

on the degree of charge transfer within each residue or group, or the

distance over which this transfer can occur.

[NOFIxed] instructs FlucQ that some or all of the bond lengths

between FlucQ-selected atoms are free to change during a simulation.

This forces the FlucQ code to recalculate the intramolecular

interaction at each step; since this is a costly calculation, the

default is to use interactions parameterised for equilibrium bond

lengths, with which it is strongly recommended to combine constraint

methods such as SHAKE BONH PARA.

The FLUCq PRINt command simply prints the current values of all

charges and charge forces (from the last energy calculation). A similar

effect can also be achieved with the standard SCALAR command (see

scalar.info for information on other FlucQ parameters available with the

SCALAR command).

The FLUCQ OFF command disables the FlucQ code. Further energy

calculations will not include FlucQ terms. Note, however, that if the

charges have been modified by FlucQ, they will remain at their altered

values.

Default behaviour during dynamics is to allow the charge degrees of

freedom to fluctuate freely; however they can be thermostatted at a given

charge "temperature" by passing extra options to the DYNAmics command:-

[FQTEmp <real>] specifies the charge temperature (default 0).

[FQTCoupling <real>] (default 0) if set, uses the Berendsen weak

coupling algorithm to thermostat the charges. The coupling parameter

is given in 1/ps, and is analagous to the TCONS/TCOU dynamics options.

[FQMAss <real>] (default 0) if set, uses Nose-Hoover thermostatting,

with the given mass. The tolerance of the Nose-Hoover iterations can be

set with FQTOlerance (default 1.0d-7), and the maximum number of

iterations with FQITerations (default 100).

Thermostatting parameters (number of iterations, scale factor, etc.)

can be written out to a given unit number at every dynamics step by using

the FQUNit (default -1: no write) option.

[FQSCal <integer>] (default 0) if set, performs simple charge velocity

scaling every FQSCal dynamics steps.

The initialization process dimensions FlucQ with the current state

of the system. The QM region, if any, is detected, and the FlucQ atom

selection will then interact with the QM region. Thus, the FLUCQ

command should be placed after any QUANTUM, CADPAC, or GAMESS command,

and if the total number of atoms in the system is modified, FlucQ

should be disabled prior to this change and reinitialized afterwards.

To skip FlucQ energy calculations entirely, use the SKIP FQPOL FQKIN

command. The QM/MM FlucQ interaction is calculated in line with the

standard QM/MM electrostatic interaction, and as such is suppressed

with the SKIP QMEL command. Finally, the intermolecular contribution

to FlucQ is calculated in line with the standard electrostatic

interaction, and so is disabled with the SKIP ELEC command.

No FlucQ interaction energies are calculated between atoms

constrained with the CONS FIX command, as electrostatic energies are

not calculated for these atoms.

FlucQ parameters are specified in the parameter file, with the FLUCQ

keyword. The section should look like the following:-

FLUCQ

atom chi zeta prin mass

Here, chi is an electronegativity measure (in Kcal/mol/e), zeta a

Slater orbital exponent (in 1/Angstrom), prin the Slater orbital

principal quantum number, and mass the charge mass (in (ps/e)**2

Kcal/mol) from the FlucQ model. For example, Rick's original

parameters for TIP4P hydrogen and M-site would be written as:-

FLUCQ

HP 10.00 0.90 1 6.0d-5

MP 78.49 1.63 2 6.0d-5

FlucQ code is enabled within CHARMM by means of the FLUCQ ON

command. Future energy calculations will then include an extra energy

term - FQPO, the FlucQ polarisation energy, while dynamics simulations

involve a new energy property - FQKI, the FlucQ charge kinetic energy.

Once FlucQ is active, the selected atoms are treated as extra degrees

of freedom, free to fluctuate under the charge forces in the system,

and, by assigning each atom type a fictional charge "mass", these

charges can be accelerated in a conventional dynamics simulation, in a

completely analogous way to the Cartesian degrees of freedom.

If atoms are selected by the FLUCQ command which cannot be modelled

(i.e. they are QM atoms, or have no FlucQ parameters defined for them)

they will be automatically removed from the selection.

The FlucQ polarisation energy, FQPO, is an intramolecular

interaction; in full electronegativity equalisation, every atom

interacts through space, by means of a modified Coulomb-type

interaction, with every other atom in the molecule. In this

implementation, the only interactions calculated are those along

defined CHARMM bonds (even those with zero force constants).

[GROUp] conserves charge within groups, rather than the default

behaviour of conserving charge within residues; this prohibits charge

transfer between groups. Note that the FlucQ model makes no restriction

on the degree of charge transfer within each residue or group, or the

distance over which this transfer can occur.

[NOFIxed] instructs FlucQ that some or all of the bond lengths

between FlucQ-selected atoms are free to change during a simulation.

This forces the FlucQ code to recalculate the intramolecular

interaction at each step; since this is a costly calculation, the

default is to use interactions parameterised for equilibrium bond

lengths, with which it is strongly recommended to combine constraint

methods such as SHAKE BONH PARA.

The FLUCq PRINt command simply prints the current values of all

charges and charge forces (from the last energy calculation). A similar

effect can also be achieved with the standard SCALAR command (see

scalar.info for information on other FlucQ parameters available with the

SCALAR command).

The FLUCQ OFF command disables the FlucQ code. Further energy

calculations will not include FlucQ terms. Note, however, that if the

charges have been modified by FlucQ, they will remain at their altered

values.

Default behaviour during dynamics is to allow the charge degrees of

freedom to fluctuate freely; however they can be thermostatted at a given

charge "temperature" by passing extra options to the DYNAmics command:-

[FQTEmp <real>] specifies the charge temperature (default 0).

[FQTCoupling <real>] (default 0) if set, uses the Berendsen weak

coupling algorithm to thermostat the charges. The coupling parameter

is given in 1/ps, and is analagous to the TCONS/TCOU dynamics options.

[FQMAss <real>] (default 0) if set, uses Nose-Hoover thermostatting,

with the given mass. The tolerance of the Nose-Hoover iterations can be

set with FQTOlerance (default 1.0d-7), and the maximum number of

iterations with FQITerations (default 100).

Thermostatting parameters (number of iterations, scale factor, etc.)

can be written out to a given unit number at every dynamics step by using

the FQUNit (default -1: no write) option.

[FQSCal <integer>] (default 0) if set, performs simple charge velocity

scaling every FQSCal dynamics steps.

The initialization process dimensions FlucQ with the current state

of the system. The QM region, if any, is detected, and the FlucQ atom

selection will then interact with the QM region. Thus, the FLUCQ

command should be placed after any QUANTUM, CADPAC, or GAMESS command,

and if the total number of atoms in the system is modified, FlucQ

should be disabled prior to this change and reinitialized afterwards.

To skip FlucQ energy calculations entirely, use the SKIP FQPOL FQKIN

command. The QM/MM FlucQ interaction is calculated in line with the

standard QM/MM electrostatic interaction, and as such is suppressed

with the SKIP QMEL command. Finally, the intermolecular contribution

to FlucQ is calculated in line with the standard electrostatic

interaction, and so is disabled with the SKIP ELEC command.

No FlucQ interaction energies are calculated between atoms

constrained with the CONS FIX command, as electrostatic energies are

not calculated for these atoms.

FlucQ parameters are specified in the parameter file, with the FLUCQ

keyword. The section should look like the following:-

FLUCQ

atom chi zeta prin mass

Here, chi is an electronegativity measure (in Kcal/mol/e), zeta a

Slater orbital exponent (in 1/Angstrom), prin the Slater orbital

principal quantum number, and mass the charge mass (in (ps/e)**2

Kcal/mol) from the FlucQ model. For example, Rick's original

parameters for TIP4P hydrogen and M-site would be written as:-

FLUCQ

HP 10.00 0.90 1 6.0d-5

MP 78.49 1.63 2 6.0d-5

Top

The FlucQ model relies on keeping charge kinetic energy at a

temperature close to zero Kelvin, to maintain Born-Oppenheimer

separation between it and the other degrees of freedom. Thus, it is

best to acquire a minimum energy charge configuration for your system

before any dynamics simulation.

Two methods are available for such "charge solution". The first is

to use a standard CHARMM minimisation; FlucQ charges will be minimised

concurrently with the Cartesian coordinates. The second method is to

apply dissipative Langevin dynamics to the charges only, to achieve

minimum energy charges for fixed atomic coordinates; this is performed

by means of the FLUCq EXACt command. The code prints a running count

of the number of iterations required to quench the kinetic energy.

[TIMEstep real] sets the timestep to be used in Langevin dynamics,

by default 0.001ps.

[ZETA real] sets the frictional coefficient, by default 1600.

[TQDEsired real] sets the desired final temperature, by default

1.0d-6 K.

[PRINt] if set, prints the final charges.

The FlucQ model relies on keeping charge kinetic energy at a

temperature close to zero Kelvin, to maintain Born-Oppenheimer

separation between it and the other degrees of freedom. Thus, it is

best to acquire a minimum energy charge configuration for your system

before any dynamics simulation.

Two methods are available for such "charge solution". The first is

to use a standard CHARMM minimisation; FlucQ charges will be minimised

concurrently with the Cartesian coordinates. The second method is to

apply dissipative Langevin dynamics to the charges only, to achieve

minimum energy charges for fixed atomic coordinates; this is performed

by means of the FLUCq EXACt command. The code prints a running count

of the number of iterations required to quench the kinetic energy.

[TIMEstep real] sets the timestep to be used in Langevin dynamics,

by default 0.001ps.

[ZETA real] sets the frictional coefficient, by default 1600.

[TQDEsired real] sets the desired final temperature, by default

1.0d-6 K.

[PRINt] if set, prints the final charges.

Top

By default, the charge polarisation energy FQPOL reported by FlucQ

is given relative to all atomic charges being zero. More generally, it

is useful to define this term relative to an arbitrary zero. This

reference energy can be set with the FLUCQ REFErence command.

FLUCQ REFE GAS disables all intermolecular interactions, solves for

exact charges, and then uses the resultant energy as the reference.

This essentially defines the polarisation energy relative to the energy

that the system would have in the gas phase, with all residues or

groups infinitely separated.

FLUCQ REFE SOLVENT merely disables the QM/MM interaction, and then

sets the reference energy similarly. This shows polarisation as a

function purely of the QM system.

FLUCQ REFE CURRent defines the current polarisation energy (from the

last energy calculation) to be zero - i.e. the reference energy is

increased by the current energy.

FLUCQ REFE ENERgy real sets the reference energy to a user-specified

value.

Bear in mind that REFE GAS exac-spec is essentially identical to the

series of CHARMM commands:-

FLUCQ REFER ENER 0

SKIP ALL EXCL FQPOL BOND ANGL UREY DIHE IMPR

FLUCQ EXACT exac-spec

FLUCQ REFER ENER ?FQPO

SKIP EXCL ALL

(The only difference is that any SKIP command in force before REFE

GAS will remain in force afterwards, whereas the above example will

re-include calculation of all energy terms at completion. Also, by

changing the second line in the above example to SKIP QMEL QMVDW, the

action of the REFE SOLVENT command can be reproduced.)

By default, the charge polarisation energy FQPOL reported by FlucQ

is given relative to all atomic charges being zero. More generally, it

is useful to define this term relative to an arbitrary zero. This

reference energy can be set with the FLUCQ REFErence command.

FLUCQ REFE GAS disables all intermolecular interactions, solves for

exact charges, and then uses the resultant energy as the reference.

This essentially defines the polarisation energy relative to the energy

that the system would have in the gas phase, with all residues or

groups infinitely separated.

FLUCQ REFE SOLVENT merely disables the QM/MM interaction, and then

sets the reference energy similarly. This shows polarisation as a

function purely of the QM system.

FLUCQ REFE CURRent defines the current polarisation energy (from the

last energy calculation) to be zero - i.e. the reference energy is

increased by the current energy.

FLUCQ REFE ENERgy real sets the reference energy to a user-specified

value.

Bear in mind that REFE GAS exac-spec is essentially identical to the

series of CHARMM commands:-

FLUCQ REFER ENER 0

SKIP ALL EXCL FQPOL BOND ANGL UREY DIHE IMPR

FLUCQ EXACT exac-spec

FLUCQ REFER ENER ?FQPO

SKIP EXCL ALL

(The only difference is that any SKIP command in force before REFE

GAS will remain in force afterwards, whereas the above example will

re-include calculation of all energy terms at completion. Also, by

changing the second line in the above example to SKIP QMEL QMVDW, the

action of the REFE SOLVENT command can be reproduced.)

Top

The fluctuating charge code alters the atomic charges during

dynamics runs. Thus, the charges cannot be treated as constant and

restart and trajectory files must include atomic charges. Files read or

written during FlucQ-enabled dynamics runs will be assumed to contain

charge information, and so will be a) somewhat larger and b)

incompatible with non-FQ files. (If FlucQ is compiled in but not

activated with FLUCQ ON, the restart and trajectory file formats are

unchanged from standard CHARMM.)

The FlucQ model is implemented primarily for the study of QM/MM

systems, with a fluctuating charge SHAKE-constrained MM solvent. Hence,

intramolecular interactions are restricted to those between FlucQ atoms

along bonds. This complicates the application of the model to large systems,

as for full electronegativity equalisation, every atom must interact with

every other atom in the group.

FlucQ is not implemented for all nonbond routines, in particular the

CFF, MMFF, CRAYVEC and PARVECT codes. FlucQ also works only with standard

Ewald, and not PME.

The fluctuating charge code alters the atomic charges during

dynamics runs. Thus, the charges cannot be treated as constant and

restart and trajectory files must include atomic charges. Files read or

written during FlucQ-enabled dynamics runs will be assumed to contain

charge information, and so will be a) somewhat larger and b)

incompatible with non-FQ files. (If FlucQ is compiled in but not

activated with FLUCQ ON, the restart and trajectory file formats are

unchanged from standard CHARMM.)

The FlucQ model is implemented primarily for the study of QM/MM

systems, with a fluctuating charge SHAKE-constrained MM solvent. Hence,

intramolecular interactions are restricted to those between FlucQ atoms

along bonds. This complicates the application of the model to large systems,

as for full electronegativity equalisation, every atom must interact with

every other atom in the group.

FlucQ is not implemented for all nonbond routines, in particular the

CFF, MMFF, CRAYVEC and PARVECT codes. FlucQ also works only with standard

Ewald, and not PME.

Top

In order for the QM/MM calculation to be properly calculated, FlucQ

requires data to be passed back to it from the QM codes (in particular

the density matrix and one-electron integrals). Changes have been made

to the QUANTUM interface for this to be carried out correctly; however,

the GAMESS(US) and CADPAC codes, not being distributed with CHARMM, will

require modification. These modifications will not affect the

functioning of standard QM/MM calculations, when FlucQ is disabled.

GAMESS-UK (versions 6.3.1 and later) should incorporate the required

modifications.

Patches for GAMESS(US), and CADPAC can be found in the

source/flucq/ directory in the main CHARMM distribution. They should be

applied in the top directory of the relevant QM code distributionm

i.e. gamess-us.patch and cadpac.patch should be applied in the

source/gamint/gamess/ and source/cadint/cadpac/ directories,

respectively. The patch files are standard unified diffs, and so should

be applied with a command similar to "patch -p1 < gamess-us.patch"

In order for the QM/MM calculation to be properly calculated, FlucQ

requires data to be passed back to it from the QM codes (in particular

the density matrix and one-electron integrals). Changes have been made

to the QUANTUM interface for this to be carried out correctly; however,

the GAMESS(US) and CADPAC codes, not being distributed with CHARMM, will

require modification. These modifications will not affect the

functioning of standard QM/MM calculations, when FlucQ is disabled.

GAMESS-UK (versions 6.3.1 and later) should incorporate the required

modifications.

Patches for GAMESS(US), and CADPAC can be found in the

source/flucq/ directory in the main CHARMM distribution. They should be

applied in the top directory of the relevant QM code distributionm

i.e. gamess-us.patch and cadpac.patch should be applied in the

source/gamint/gamess/ and source/cadint/cadpac/ directories,

respectively. The patch files are standard unified diffs, and so should

be applied with a command similar to "patch -p1 < gamess-us.patch"

Top

The following example initialises the FlucQ code for a system of SPC

waters, before calculating the gas phase energy, and then calculating

the self-polarisation of the solvent. Finally, the total energy,

including the self-polarisation relative to the gas phase, is printed,

and the charge forces from this energy calculation are displayed.

FLUCQ ON SELE RESN SPC END

FLUCQ REFER GAS

FLUCQ EXACT

ENERGY

SCALAR FQCFOR SHOW SELE ALL END

See the testcase test/c28test/fqam1.inp for an example of a FlucQ

dynamics simulation.

The following example initialises the FlucQ code for a system of SPC

waters, before calculating the gas phase energy, and then calculating

the self-polarisation of the solvent. Finally, the total energy,

including the self-polarisation relative to the gas phase, is printed,

and the charge forces from this energy calculation are displayed.

FLUCQ ON SELE RESN SPC END

FLUCQ REFER GAS

FLUCQ EXACT

ENERGY

SCALAR FQCFOR SHOW SELE ALL END

See the testcase test/c28test/fqam1.inp for an example of a FlucQ

dynamics simulation.

Top

The standard CHARMM nonbond routines and QM codes have been modified

so as to sum the interaction electrostatic interaction energy between

charge "I" and all other nonbond pairs or QM atoms into index "I" of

the fluctuating charge array FQCFOR. The FlucQ model actually requires

the term dE/dQ, so these totals are divided by charge by the FlucQ

energy routine (as all such interactions are linear in charge). Note

that this gives erroneous results for FlucQ sites with exactly zero

charge; however, the CHARMM nonbond routines calculate no interactions

for such systems anyway.

Finally, the intramolecular terms, as contributions to dE/dQ, are

summed into the FQCFOR array, and charge forces are calculated from

these electronegativities by mass-weighted averaging over residues or

groups. These forces are then used by the standard minimisers, or by a

standard Verlet integrator during dynamics.

For further information, see the following:-

MM system; (Rick et. al., J. Chem. Phys. 101 (7) 1994 p6141)

QM/MM interaction; (Bryce et. al., Chem. Phys. Lett. 279 1997, p367)

Tag Table:

Node: Top103

Node: Syntax1371

Node: Activation2114

Node: Charge solution6634

Node: Reference energy7793

Node: Caveats9466

Node: Using FlucQ with QM10631

Node: Examples15843

Node: Implementation16424

End Tag Table

The standard CHARMM nonbond routines and QM codes have been modified

so as to sum the interaction electrostatic interaction energy between

charge "I" and all other nonbond pairs or QM atoms into index "I" of

the fluctuating charge array FQCFOR. The FlucQ model actually requires

the term dE/dQ, so these totals are divided by charge by the FlucQ

energy routine (as all such interactions are linear in charge). Note

that this gives erroneous results for FlucQ sites with exactly zero

charge; however, the CHARMM nonbond routines calculate no interactions

for such systems anyway.

Finally, the intramolecular terms, as contributions to dE/dQ, are

summed into the FQCFOR array, and charge forces are calculated from

these electronegativities by mass-weighted averaging over residues or

groups. These forces are then used by the standard minimisers, or by a

standard Verlet integrator during dynamics.

For further information, see the following:-

MM system; (Rick et. al., J. Chem. Phys. 101 (7) 1994 p6141)

QM/MM interaction; (Bryce et. al., Chem. Phys. Lett. 279 1997, p367)

Tag Table:

Node: Top103

Node: Syntax1371

Node: Activation2114

Node: Charge solution6634

Node: Reference energy7793

Node: Caveats9466

Node: Using FlucQ with QM10631

Node: Examples15843

Node: Implementation16424

End Tag Table