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Department of Chemistry




The Effective Fragment Molecular Orbital Method:
  The development and application of a parameter free force field


Casper Steinmann
Department of Chemistry
University of Copenhagen




 Supervisor: Professor Jan H. Jensen




University of Copenhagen, Feb. 12th, 2013
Dias 1
Department of Chemistry




Outline

•    Motivation
•    Current approaches to treat large systems
•    My work
      •  Applications
•    Conclusions and Outlook




University of Copenhagen, Feb. 12th, 2013
Dias 2
Department of Chemistry




Motivation

•    Understand and improve enzyme catalysis

•    Large systems are problematic in a computer

•    Not one go-to program




                                KE Ranaghan, AJ Mulholland (2010), Int. Rev. Phys. Chem.

University of Copenhagen, Feb. 12th, 2013
Dias 3
Department of Chemistry




Current approaches to treat large systems




                                               QM/MM


                                            Fragment Based
           QM                                   Method
                                                             MM


                                     And the other ones …




University of Copenhagen, Feb. 12th, 2013
Dias 4
Department of Chemistry




I want to study interaction energies …




University of Copenhagen, Feb. 12th, 2013
Dias 5
Department of Chemistry




Effective Fragment Potential Method (EFP2)

•  EFP2 is a model potential derived from first principles
    •  Multipole moments
    •  Dipole polarizability tensors
    •  Among others …




                                            doi: 10.1063/1.472045
                                            doi: 10.1021/jp002747h
University of Copenhagen, Feb. 12th, 2013
Dias 6
Department of Chemistry




Effective Fragment Potential Method (EFP2)

                                     N          N
         E   EFP 2
                     =E    HF
                                − ∑ E = ∑ ( EIJ + EIJ + EIJ ) + Etot
                                            0
                                            I
                                             ES    XR    CT       POL

                                     I          IJ




University of Copenhagen, Feb. 12th, 2013
Dias 7
Department of Chemistry




      The Effective Fragment Potential Method (EFP2)

                                           N      N
               E   EFP 2
                           =E    HF
                                      − ∑ EI = ∑ ( EIJ + EIJ + EIJ ) + Etot
                                                    ES    XR    CT       POL

                                           I      IJ




Many-body polarization

 Computed classically
 using induced dipoles
   for entire system




      University of Copenhagen, Feb. 12th, 2013
      Dias 8
Department of Chemistry




I want interaction energies and internal energies …




University of Copenhagen, Feb. 12th, 2013
Dias 9
Department of Chemistry




Fragment Based Methods
                             Fragment Molecular Orbital (FMO2)
                           And most other fragmentation methods
                                            N   N
                              E FMO2 = ∑ EI + ∑ (EIJ − EI − EJ )
                                            I   IJ




University of Copenhagen, Feb. 12th, 2013
Dias 10
Department of Chemistry




     Fragment Based Methods
                                  Fragment Molecular Orbital (FMO2)
                                And most other fragmentation methods
                                                 N   N
                                   E FMO2 = ∑ EI + ∑ (EIJ − EI − EJ )
                                                 I   IJ




Many-body Polarization:

  Monomer SCF in the
  Coulomb field of all
   other monomers

      Iterated to
    self-consistency




     University of Copenhagen, Feb. 12th, 2013
     Dias 11
Department of Chemistry




    Fragment Based Methods

                                                N   N
                                  E FMO2 = ∑ EI + ∑ (EIJ − EI − EJ )
                                                I   IJ




Non-Coulomb effects:

  Dimer SCF in the
 Coulomb field of all
  other monomers

     Iterated to
   self-consistency




    University of Copenhagen, Feb. 12th, 2013
    Dias 12
Department of Chemistry




    Fragment Based Methods

                                                N   N
                                  E FMO2 = ∑ EI + ∑ (EIJ − EI − EJ )
                                                I   IJ




 Coulomb effects:

Coulomb energy in the
 Coulomb field of all
  other monomers




    University of Copenhagen, Feb. 12th, 2013
    Dias 13
Department of Chemistry




Fragment Based Methods

•    The FMO2 method
      •  All monomers converge in the Coulomb field of all other
         monomers iteratively.
      •  Dimers converge in the static Coulomb field




University of Copenhagen, Feb. 12th, 2013
Dias 14
Department of Chemistry




I want interaction energies and internal energies …




                                            FAST




University of Copenhagen, Feb. 12th, 2013
Dias 15
Department of Chemistry




      Fragment Based Methods


                          N             RI ,J ≤Rcut                                RI ,J >Rcut

         E EFMO = ∑ EI0 +                 ∑           (EIJ − EI0 − EJ0 − EIJ ) +
                                                        0                 POL
                                                                                     ∑            ES    POL
                                                                                                 EIJ +Etot
                           I                IJ                                         IJ




  Monomer SCF in the
      gas phase


   Extract multipoles,
and dipole polarizabilities




                                                            PLoS ONE 2012, 7:e41117
      University of Copenhagen, Feb. 12th, 2013
      Dias 16
Department of Chemistry




      Fragment Based Methods


                          N             RI ,J ≤Rcut                                RI ,J >Rcut

         E EFMO = ∑ EI0 +                 ∑           (EIJ − EI0 − EJ0 − EIJ ) +
                                                        0                 POL
                                                                                     ∑            ES    POL
                                                                                                 EIJ +Etot
                           I                IJ                                         IJ




Many-body polarization

 Computed classically
 using induced dipoles
   for entire system




      University of Copenhagen, Feb. 12th, 2013
      Dias 17
Department of Chemistry




  Fragment Based Methods - EFMO


                      N             RI ,J ≤Rcut                                RI ,J >Rcut

     E EFMO = ∑ EI0 +                 ∑           (EIJ − EI0 − EJ0 − EIJ ) +
                                                    0                 POL
                                                                                 ∑            ES    POL
                                                                                             EIJ +Etot
                       I                IJ                                         IJ




   Coulomb and
Non-Coulomb effects

  dimer SCF in the
     gas phase




  University of Copenhagen, Feb. 12th, 2013
  Dias 18
Department of Chemistry




Fragment Based Methods - EFMO


                    N             RI ,J ≤Rcut                                RI ,J >Rcut

   E EFMO = ∑ EI0 +                 ∑           (EIJ − EI0 − EJ0 − EIJ ) +
                                                  0                 POL
                                                                               ∑            ES    POL
                                                                                           EIJ +Etot
                     I                IJ                                         IJ




Coulomb effects

Computed using
static multipoles




University of Copenhagen, Feb. 12th, 2013
Dias 19
Department of Chemistry




Fragment Based Methods - EFMO
                         N                  RI ,J ≤Rcut

          E COR = ∑ EICOR +                   ∑           (EIJ − EICOR − EJ ) +0
                                                            COR           COR

                         I                      IJ




University of Copenhagen, Feb. 12th, 2013
Dias 20
Department of Chemistry




Covalent Fragmentation - EFMO




University of Copenhagen, Feb. 12th, 2013   PLoS ONE 2012, 7:e41117
Dias 21
Department of Chemistry




Software to help setup calculations: FragIt

•    Use SMARTS to find places to break bonds




                                            PLoS ONE 2012, 7:e44480
University of Copenhagen, Feb. 12th, 2013
Dias 22
Department of Chemistry




Software to help setup calculations: FragIt

•    Use SMARTS to find places to break bonds


                                                        Chignolin (10 residues)




                                            PLoS ONE 2012, 7:e44480
University of Copenhagen, Feb. 12th, 2013
Dias 23
Department of Chemistry




      Fragment Based Methods - EFMO Gradients

                                                  Trp cage (20 residues)
                                                   2 residues/fragment




                                           EFMO       FMO2
Error in energy                             -4.3        6.4 kcal/mol

MP2/6-31G(d) gradient           314                     409 minutes
20 cores
(most time spent in MP2 dimers)




                                            PLoS ONE 2012, 7:e41117
      University of Copenhagen, Feb. 12th, 2013
      Dias 24
Department of Chemistry




Fragment Based Methods - EFMO QM/”MM”

                               E EFMO = EA + EA / F + EF
                              RA,J ≤Rcut                                 RA,J >Rcut

       E   EFMO
                  =E +  0
                        A       ∑ (E        0
                                            AJ
                                                   0   0
                                                 −E −E −E
                                                   A   J
                                                              POL
                                                              AJ    )+       ∑          ES     POL
                                                                                      E AJ + Etot
                                J∈F                                        J∈F




                                                                    Active




                                                                              Frozen




University of Copenhagen, Feb. 12th, 2013                  arxiv.org/abs/1212.6172
Dias 25
Department of Chemistry




     Proof of concept – chorismate mutase




ONIOM: MP2/cc-pVDZ:EFMO-RHF/6-31G(d)




                                                             16 Å

  ΔH ≠ = 18 vs 13 (exp) kcal/mol



     University of Copenhagen, Feb. 12th, 2013   arxiv.org/abs/1212.6172
     Dias 26
Department of Chemistry




Conclusion and Outlook

•    Fast polarizable force field
•    Applicable to any system



EFMO/PCM
Fully flexible EFPs
                     N        RI ,J ≤Rcut                               RI ,J >Rcut

      E   FIEFMO
                   = ∑E + 0
                          I     ∑             0    0   0
                                            (E − E − E − E
                                              IJ   I   J
                                                             POL
                                                             IJ    )+     ∑             ES    CT    XR    Disp    POL
                                                                                      (EIJ + EIJ + EIJ + EIJ ) +Etot
                     I            IJ                                        IJ




Combine MP2:RHF-D optimization




University of Copenhagen, Feb. 12th, 2013
Dias 27
Department of Chemistry




Acknowledgements

•    Jan Jensen
•    Dmitri Fedorov, AIST, Japan
•    Colleagues at the Department of Chemistry
•    Friends and Family
•    In silico Rational Engineering of Novel Enzymes (IRENE)




University of Copenhagen, Feb. 12th, 2013
Dias 28
Department of Chemistry




University of Copenhagen, Feb. 12th, 2013
Dias 29
Department of Chemistry




                                  Thank you for listening




University of Copenhagen, Feb. 12th, 2013
Dias 30

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PhD defence presentation

  • 1. Department of Chemistry The Effective Fragment Molecular Orbital Method: The development and application of a parameter free force field Casper Steinmann Department of Chemistry University of Copenhagen Supervisor: Professor Jan H. Jensen University of Copenhagen, Feb. 12th, 2013 Dias 1
  • 2. Department of Chemistry Outline •  Motivation •  Current approaches to treat large systems •  My work •  Applications •  Conclusions and Outlook University of Copenhagen, Feb. 12th, 2013 Dias 2
  • 3. Department of Chemistry Motivation •  Understand and improve enzyme catalysis •  Large systems are problematic in a computer •  Not one go-to program KE Ranaghan, AJ Mulholland (2010), Int. Rev. Phys. Chem. University of Copenhagen, Feb. 12th, 2013 Dias 3
  • 4. Department of Chemistry Current approaches to treat large systems QM/MM Fragment Based QM Method MM And the other ones … University of Copenhagen, Feb. 12th, 2013 Dias 4
  • 5. Department of Chemistry I want to study interaction energies … University of Copenhagen, Feb. 12th, 2013 Dias 5
  • 6. Department of Chemistry Effective Fragment Potential Method (EFP2) •  EFP2 is a model potential derived from first principles •  Multipole moments •  Dipole polarizability tensors •  Among others … doi: 10.1063/1.472045 doi: 10.1021/jp002747h University of Copenhagen, Feb. 12th, 2013 Dias 6
  • 7. Department of Chemistry Effective Fragment Potential Method (EFP2) N N E EFP 2 =E HF − ∑ E = ∑ ( EIJ + EIJ + EIJ ) + Etot 0 I ES XR CT POL I IJ University of Copenhagen, Feb. 12th, 2013 Dias 7
  • 8. Department of Chemistry The Effective Fragment Potential Method (EFP2) N N E EFP 2 =E HF − ∑ EI = ∑ ( EIJ + EIJ + EIJ ) + Etot ES XR CT POL I IJ Many-body polarization Computed classically using induced dipoles for entire system University of Copenhagen, Feb. 12th, 2013 Dias 8
  • 9. Department of Chemistry I want interaction energies and internal energies … University of Copenhagen, Feb. 12th, 2013 Dias 9
  • 10. Department of Chemistry Fragment Based Methods Fragment Molecular Orbital (FMO2) And most other fragmentation methods N N E FMO2 = ∑ EI + ∑ (EIJ − EI − EJ ) I IJ University of Copenhagen, Feb. 12th, 2013 Dias 10
  • 11. Department of Chemistry Fragment Based Methods Fragment Molecular Orbital (FMO2) And most other fragmentation methods N N E FMO2 = ∑ EI + ∑ (EIJ − EI − EJ ) I IJ Many-body Polarization: Monomer SCF in the Coulomb field of all other monomers Iterated to self-consistency University of Copenhagen, Feb. 12th, 2013 Dias 11
  • 12. Department of Chemistry Fragment Based Methods N N E FMO2 = ∑ EI + ∑ (EIJ − EI − EJ ) I IJ Non-Coulomb effects: Dimer SCF in the Coulomb field of all other monomers Iterated to self-consistency University of Copenhagen, Feb. 12th, 2013 Dias 12
  • 13. Department of Chemistry Fragment Based Methods N N E FMO2 = ∑ EI + ∑ (EIJ − EI − EJ ) I IJ Coulomb effects: Coulomb energy in the Coulomb field of all other monomers University of Copenhagen, Feb. 12th, 2013 Dias 13
  • 14. Department of Chemistry Fragment Based Methods •  The FMO2 method •  All monomers converge in the Coulomb field of all other monomers iteratively. •  Dimers converge in the static Coulomb field University of Copenhagen, Feb. 12th, 2013 Dias 14
  • 15. Department of Chemistry I want interaction energies and internal energies … FAST University of Copenhagen, Feb. 12th, 2013 Dias 15
  • 16. Department of Chemistry Fragment Based Methods N RI ,J ≤Rcut RI ,J >Rcut E EFMO = ∑ EI0 + ∑ (EIJ − EI0 − EJ0 − EIJ ) + 0 POL ∑ ES POL EIJ +Etot I IJ IJ Monomer SCF in the gas phase Extract multipoles, and dipole polarizabilities PLoS ONE 2012, 7:e41117 University of Copenhagen, Feb. 12th, 2013 Dias 16
  • 17. Department of Chemistry Fragment Based Methods N RI ,J ≤Rcut RI ,J >Rcut E EFMO = ∑ EI0 + ∑ (EIJ − EI0 − EJ0 − EIJ ) + 0 POL ∑ ES POL EIJ +Etot I IJ IJ Many-body polarization Computed classically using induced dipoles for entire system University of Copenhagen, Feb. 12th, 2013 Dias 17
  • 18. Department of Chemistry Fragment Based Methods - EFMO N RI ,J ≤Rcut RI ,J >Rcut E EFMO = ∑ EI0 + ∑ (EIJ − EI0 − EJ0 − EIJ ) + 0 POL ∑ ES POL EIJ +Etot I IJ IJ Coulomb and Non-Coulomb effects dimer SCF in the gas phase University of Copenhagen, Feb. 12th, 2013 Dias 18
  • 19. Department of Chemistry Fragment Based Methods - EFMO N RI ,J ≤Rcut RI ,J >Rcut E EFMO = ∑ EI0 + ∑ (EIJ − EI0 − EJ0 − EIJ ) + 0 POL ∑ ES POL EIJ +Etot I IJ IJ Coulomb effects Computed using static multipoles University of Copenhagen, Feb. 12th, 2013 Dias 19
  • 20. Department of Chemistry Fragment Based Methods - EFMO N RI ,J ≤Rcut E COR = ∑ EICOR + ∑ (EIJ − EICOR − EJ ) +0 COR COR I IJ University of Copenhagen, Feb. 12th, 2013 Dias 20
  • 21. Department of Chemistry Covalent Fragmentation - EFMO University of Copenhagen, Feb. 12th, 2013 PLoS ONE 2012, 7:e41117 Dias 21
  • 22. Department of Chemistry Software to help setup calculations: FragIt •  Use SMARTS to find places to break bonds PLoS ONE 2012, 7:e44480 University of Copenhagen, Feb. 12th, 2013 Dias 22
  • 23. Department of Chemistry Software to help setup calculations: FragIt •  Use SMARTS to find places to break bonds Chignolin (10 residues) PLoS ONE 2012, 7:e44480 University of Copenhagen, Feb. 12th, 2013 Dias 23
  • 24. Department of Chemistry Fragment Based Methods - EFMO Gradients Trp cage (20 residues) 2 residues/fragment EFMO FMO2 Error in energy -4.3 6.4 kcal/mol MP2/6-31G(d) gradient 314 409 minutes 20 cores (most time spent in MP2 dimers) PLoS ONE 2012, 7:e41117 University of Copenhagen, Feb. 12th, 2013 Dias 24
  • 25. Department of Chemistry Fragment Based Methods - EFMO QM/”MM” E EFMO = EA + EA / F + EF RA,J ≤Rcut RA,J >Rcut E EFMO =E + 0 A ∑ (E 0 AJ 0 0 −E −E −E A J POL AJ )+ ∑ ES POL E AJ + Etot J∈F J∈F Active Frozen University of Copenhagen, Feb. 12th, 2013 arxiv.org/abs/1212.6172 Dias 25
  • 26. Department of Chemistry Proof of concept – chorismate mutase ONIOM: MP2/cc-pVDZ:EFMO-RHF/6-31G(d) 16 Å ΔH ≠ = 18 vs 13 (exp) kcal/mol University of Copenhagen, Feb. 12th, 2013 arxiv.org/abs/1212.6172 Dias 26
  • 27. Department of Chemistry Conclusion and Outlook •  Fast polarizable force field •  Applicable to any system EFMO/PCM Fully flexible EFPs N RI ,J ≤Rcut RI ,J >Rcut E FIEFMO = ∑E + 0 I ∑ 0 0 0 (E − E − E − E IJ I J POL IJ )+ ∑ ES CT XR Disp POL (EIJ + EIJ + EIJ + EIJ ) +Etot I IJ IJ Combine MP2:RHF-D optimization University of Copenhagen, Feb. 12th, 2013 Dias 27
  • 28. Department of Chemistry Acknowledgements •  Jan Jensen •  Dmitri Fedorov, AIST, Japan •  Colleagues at the Department of Chemistry •  Friends and Family •  In silico Rational Engineering of Novel Enzymes (IRENE) University of Copenhagen, Feb. 12th, 2013 Dias 28
  • 29. Department of Chemistry University of Copenhagen, Feb. 12th, 2013 Dias 29
  • 30. Department of Chemistry Thank you for listening University of Copenhagen, Feb. 12th, 2013 Dias 30