Upload
others
View
2
Download
0
Embed Size (px)
Citation preview
QUANTUM MECHANICAL EFFECTS FROM RING POLYMER MOLECULAR DYNAMICS
Department of Chemical Engineering, Massachusetts Institute of Technology
77 Massachusetts Avenue, Cambridge, MA 02139
01.26.2013
2005 MSc in Chemistry (Moscow State University) 2009 PhD in Theoretical Chemistry (Moscow State University) 2009-11 Newton International Fellow (Royal Society/University of Oxford) 2011- Princeton CEFRC Fellow (Princeton/MIT)
Dr. Yury V. Suleymanov
Outline
1. Ring polymer molecular dynamics 2. Ring polymer reaction rate theory • Chemical reactions: - A+BC (H+H2, Cl+HCl, F+H2,Mu+ H2) - H+CH4
3. RPMDrate code
1. Ring polymer molecular dynamics Based on the classical isomorphism:a
][ HetrZ β−=∫ ∫ −= ),(
)2(1
nnnnHnnn eddZ qpqp β
πwhere
a D. Chandler and P. G. Wolynes, JCP 74, 4078 (1981). ./1 and /with
)()(21
2),(
1
21
22
nnn
n
jjjjn
jnnn
n
qVqqmm
pH
βωββ
ω
==
+−+=∑
=−qp
Single quantum particle
Classical n-bead ring polymer
)ˆ(2ˆ
)ˆ,ˆ(2
qVm
pqpH +=
QM partition function: Classical partition function:
where
map each quantum particle onto an effective classical system of N beads coupled via harmonic springs and each under external potential V
∞→n
1. Ring polymer molecular dynamics Based on the classical isomorphism:a
][ HetrZ β−=∫ ∫ −= ),(
)2(1
nnnnHnnn eddZ qpqp β
πwhere
a D. Chandler and P. G. Wolynes, JCP 74, 4078 (1981). ./1 and /with
)()(21
2),(
1
21
22
nnn
n
jjjjn
jnnn
n
qVqqmm
pH
βωββ
ω
==
+−+=∑
=−qp
Single quantum particle
Classical n-bead ring polymer
)ˆ(2ˆ
)ˆ,ˆ(2
qVm
pqpH +=
QM partition function: Classical partition function:
where
map each quantum particle onto an effective classical system of N beads coupled via harmonic springs and each under external potential V
∞→n π8/)(TRG Λ=
mkThT π2/)( =Λ
(Proof) [ ] ( )[ ] ./ where, netretrZ n
nHH n ββββ === −−
,1211 qeqqeqdqdqZ Hn
Hn
nn ββ −−∫∫=
So
where
∫ −−−− −= )(/)(2/ 12
21 jnjjn qVqqipmpdpe ββ
π
[ ])(2/)(2/1
21
2221 jjjnn qVqqm
n
em +−− −
= ωβ
βπ
π
[ ] ann
qVqqmmpj
jjjnjnedp ./1 with ,21 )(2/)(2/ 2
122
βωπ
ωβ =≡ +−+− −∫
a M. Parrinello and A. Rahman, JCP 80, 860 (1984).
Path Integral Molecular Dynamics (PIMD) • The ring polymer trajectories
as a sampling tool to calculate exact values of static equilibrium properties such as
[ ].1 AetrZ
A Hβ−=
pn
qn
Note: - any classical method (MC, MD) can be used to sample multidimendional
configuration integrals: PIMD - Molecular Dynamics - PIMD: Time is only a parameter for the exploration of phase space
(considered as unphysical dynamics).
Examples: • thermodynamic energy • heat capacity • Helmholtz free energy
ββ
∂∂
−=)(ln ZE
2
2
2B
ln1β∂
∂=
∂∂
=Z
TkTE
Cv
ZTkF lnB−=
Ring Polymer Molecular Dynamics (RPMD)
The RPMD approximation is simply:
,)()()2(
1)(~0
),(00
00∫ ∫ −≈ tnnH
nAB BAeddZ
tc nn qqqp qpβ
π
where
.)(1)( and )(1)(11∑∑==
==n
jjn
n
jjn qB
nBqA
nA qq
(Classical molecular dynamics in an extended phase space)
pn
qn
• The same ring polymer trajectories to calculate approximate Kubo-transformed correlation functions of the form
[ ].)()0(1)(~0
)(∫ −−−=β
λλβλβ
tBeAetrdZ
tc HHAB
.)()(1)(0∫ −=β
λλβ
thiFtrdtc ),(lim)(
1)( side-flux tcTQ
Tkt
r∞→
=
).( TSqq −= hh
Examples: • Chemical reaction rates
Step operator: Flux operator:
• Diffusion coefficients ,)(1)(
0velocity-velocity∫
∞
= dttcd
TD .)()(1)(0∫ −=β
λλβ
tmpi
mptrdtc
• Neutron scattering ,),(
21),(
functionscattering
teintermedia
structuredynamicincoherent dttkFewkS iwt∫
∞
∞−
−=π
,1),(particle
1
)()(
0particle∑∫=
⋅+−⋅−=N
j
tiii jj eedN
tkF rkrk λβ
λβ
- energy transfer (from neutron to liquid)
- momentum transfer jie rk⋅− )(ti je rk⋅+and - correlated density operators
• Dipole absorption spectroscopy
),(Volume3
)()(0
2
wIc
wwwnε
πβα =
∫+∞
∞−−
−−−
= ),(2
)1()( tCdtew
ewI dipoledipoleiwt
w
πβ
β,)()(1)(
0∫ −=β
µλµλβ
tidtC
,)( )( HH eeiF λλβλ −−−≡− F,)( // iHtiHt eeth −+≡ h
)(wα)(wn
- Beer-Lambert absorption coefficient
- frequency-dependent refraction index
Golden rule of TDPT:
Properties of RPMD:
1. Exact in the limit as t → 0.a 2. Exact in the classical (high temperature) limit.b
3. Exact in the harmonic limit (for linear A and/or B).b
4. Exact when A = 1 (the unit operator).c
5. Consistent with the QM equilibrium distribution.
a B. J. Braams and D. E. Manolopoulos, JCP 125, 124105 (2006). b I. R. Craig and D. E. Manolopoulos, JCP 121, 3368 (2004). c S. Habershon and D. E. Manolopoulos, JCP 131, 244518 (2009).
(exact QM rate coefficient for a parabolic barrier)
(exact QM in the low T limit)
𝑍 = 𝑒−𝛽𝐸0
RPMD:
(exact QM rate coefficient for a parabolic barrier)
(exact QM in the low T limit)
𝑍 = 𝑒−𝛽𝐸0
RPMD: But it neglects QM interference effects in the real-time dynamics (no 𝑒±𝑖𝑖𝑖/ℏ)
Example applications:
1. Quantum diffusion in liquid para-hydrogen (2005). 2. Quantum diffusion in liquid water (2005). 3. Neutron scattering from liquid para-hydrogen (2006). 4. Proton transfer in a polar solvent (2008). 5. Diffusion of H isotopes in water and ice (2008). 6. Dynamics of the solvated electron (2008). 7. Diffusion of H isotopes in transition metals (2009). 8. Competing quantum effects in liquid water (2009). 9. Hydrogen surface diffusion (2012). 10. Gas phase chemical reaction rates (2009-2012).
Example applications:
1. Quantum diffusion in liquid para-hydrogen (2005). 2. Quantum diffusion in liquid water (2005). 3. Neutron scattering from liquid para-hydrogen (2006). 4. Proton transfer in a polar solvent (2008). 5. Diffusion of H isotopes in water and ice (2008). 6. Dynamics of the solvated electron (2008). 7. Diffusion of H isotopes in transition metals (2009). 8. Competing quantum effects in liquid water (2009). 9. Hydrogen surface diffusion (2012). 10. Gas phase chemical reaction rates (2009-2012).
2. Ring polymer reaction rate theory Consider an atom-diatom reaction in the gas phase
A+BC→AB+C The exact QM rate coefficient is
),(~lim)(
1)( stcTQ
Tk fstr
∞→=
where
[ ].)()0(1),(~0
)(∫ −−−=β
λλβλβ
theFetrdstc HHfs
with
[ ]
=≡=0>s ,10<s ,0
)( and , shhhHiF
(Flux) (Side) NB: 1. k(T) is independent of s 2. cfs(t→0+)~0
2. Ring polymer reaction rate theory The classical limit rate coefficient is
),(lim)(
1)( stcTQ
Tk clfst
r
cl
∞→=
where
[ ] [ ]
)()()(
)2(1);(
00
),(
0000
t
Hfff
cl
shdt
dss
eddstcfs
qqq
qpqp
××
=−
∫ ∫
δ
πβ
Flux (t = 0) Side (t > 0) NB: 1. kcl(T) is independent of s 2. cfs(t→0+)≠0 → classical TST
2. Ring polymer reaction rate theory The RPDM rate coefficient is
);(lim)(
1)( stcTQ
Tk fstr
RPMD
∞→=
where
[ ] [ ]
)()()(
)2(1);(
00
),(
0000
t
Hnfnfnffs
shdt
dss
eddstc nn
qqq
qp qp
××
= −∫ ∫
δ
πβ
Flux (t = 0) Side (t > 0)
nnn
n
jjjjn
jn nqVqqm
mp
H βωββω /1 ,/ with ,)()(21
2),(
1
21
22
==
+−+=∑
=−qp
and
∑∑==
==n
jj
n
jj p
npq
nq
11
1 ,1
NB: 1. kRPMD(T) is independent of s 2. cfs(t→0+)≠0 → “quantum” TST (centroid density)
Computational strategy
0)(0 =qs
0)(1 =qs
- dividing surface in the asymptotic reactant valley
- dividing surface in the region of the reaction barrier
Computational strategy
0)(0 =qs
0)(1 =qs
- dividing surface in the asymptotic reactant valley
- dividing surface in the region of the reaction barrier
)(
0
),(
0
1
)(
1
1
0011
)();0(
);0();0(
);0();(
)(
sk
r
fs
ssp
fs
fs
s
fs
fsRPMD
QTST
TQstc
stcstc
stcstc
Tk +
+
+
+
→×
→
→×
→
∞→=
κ
Computational strategy
0)(0 =qs
0)(1 =qs
- dividing surface in the asymptotic reactant valley
- dividing surface in the region of the reaction barrier
)(
0
),(
0
1
)(
1
1
0011
)();0(
);0();0(
);0();(
)(
sk
r
fs
ssp
fs
fs
s
fs
fsRPMD
QTST
TQstc
stcstc
stcstc
Tk +
+
+
+
→×
→
→×
→
∞→=
κ
transmission coefficient for s1
kQTST(s0) ratio of ring polymer averages on two different dividing surfaces
Computational strategy
0)(0 =qs
0)(1 =qs
- dividing surface in the asymptotic reactant valley
- dividing surface in the region of the reaction barrier
)(
0
),(
0
1
)(
1
1
0011
)();0(
);0();0(
);0();(
)(
sk
r
fs
ssp
fs
fs
s
fs
fsRPMD
QTST
TQstc
stcstc
stcstc
Tk +
+
+
+
→×
→
→×
→
∞→=
κ
Rq −= ∞Rs )(0
2/12
0 214)(
= ∞
R
QTST Rskπβµ
π
Consider the following dividing surface s0
CBA
CBAR
ACB
CcBB
mmmmmm
,mmmm
CABBCA
+++
=
−++
=
+→+
)(µ
rrrR
Computational strategy
0)(0 =qs
0)(1 =qs
- dividing surface in the asymptotic reactant valley
- dividing surface in the region of the reaction barrier
2/12
),(
0
1
)(
1
1
214
);0();0(
);0();(
)(
011
×
→
→×
→
∞→= ∞
+
+
+ R
ssp
fs
fs
s
fs
fsRPMD Rstcstc
stcstc
Tkπβµ
π
κ
Two separate stages:
1. Calculate κ(s1) (dynamical) 2. Calculate p(s1,s0) (static)
Computational strategy
0)(0 =qs
0)(1 =qs
- dividing surface in the asymptotic reactant valley
- dividing surface in the region of the reaction barrier
Advantages: 1. Practical way to compute k(T) when the probability that a spontaneous thermal fluctuation will bring the system to the TS is very small 2. No need to calculate Qr(T)
2/12
),(
0
1
)(
1
1
214
);0();0(
);0();(
)(
011
×
→
→×
→
∞→= ∞
+
+
+ R
ssp
fs
fs
s
fs
fsRPMD Rstcstc
stcstc
Tkπβµ
π
κ
Computational strategy
1
1
1
)]([)()();0();(
1011
0
)(
1
1 lims
tst
s
fs
fs shdt
dsfstcstc
qqq −
∞→+
=→
∞→
κ
0)(0 =qs
0)(1 =qs
- dividing surface in the asymptotic reactant valley
- dividing surface in the region of the reaction barrier
2/163
1
2)(
21)(
∂∂
= ∑−
=
N
i iis q
sf qqπβµ
where
Computational strategy
0)(0 =qs
0)(1 =qs
- dividing surface in the asymptotic reactant valley
- dividing surface in the region of the reaction barrier
)]0()1([
),(
0
1
01
);0();0( WW
ssp
fs
fs estcstc −−
+
+ =→
→ β
W(ξ) is the centroid potential of mean force along the reaction coordinate
==
=−
=0)( ,0
0)( ,1)()(
)(0
1
10
0
qqq
ss
sssξ
Umbrella integration along the reaction coordinate:
• H + H2 • D + H2 • Mu + H2
• H + CH4 • D + CH4 • Mu + CH4 • O + CH4
• Cl + HCl • F + H2
RESULTS: H+H2
Classical and RPMD potentials of mean force for the H+H2 reaction at 1000 and 300 K.
Classical (dashed) and RPMD (solid) transmission coefficients for the H+H2 reaction at 1000 and 300 K.
R. Collepardo-Guevara, Yu. V. Suleimanov, and D. E. Manolopoulos, J. Chem. Phys. (2009) 130, 174713.
RESULTS: H+H2
Arrhenius plot of quantum, RPMD, and classical rate coefficients for the distinguishable atom H+H2 reaction between 200 and 1500 K (quantum results stopping at 1000 K).
Deep quantum tunnelling • RPMD gives k(T) within a factor of 2 of the exact QM result when the classical rate is out by 3 orders of magnitude
Symmetric barrier. Tc = 345 K.
R. Collepardo-Guevara, Yu. V. Suleimanov, and D. E. Manolopoulos, J. Chem. Phys. (2009) 130, 174713.
RESULTS: Cl+HCl
Classical and RPMD potentials of mean force for the Cl+HCl reaction at 1000 and 300 K
Classical (dashed) and RPMD (solid) transmission coefficients for the Cl+HCl reaction at 1000 and 300 K.
R. Collepardo-Guevara, Yu. V. Suleimanov, and D. E. Manolopoulos, J. Chem. Phys. (2009) 130, 174713.
RESULTS: Cl+HCl
Arrhenius plot of quantum, RPMD, and classical rate coefficients for the Cl+HCl reaction between 200 and 1500 K (quantum results stopping at 1000 K).
Symmetric barrier. Tc = 320 K.
R. Collepardo-Guevara, Yu. V. Suleimanov, and D. E. Manolopoulos, J. Chem. Phys. (2009) 130, 174713.
RESULTS: F+H2
Classical and RPMD potentials of mean force for the F+H2 reaction at 1000 and 300 K
Classical (dashed) and RPMD (solid) transmission coefficients for the F+H2 reaction at 1000 and 300 K.
R. Collepardo-Guevara, Yu. V. Suleimanov, and D. E. Manolopoulos, J. Chem. Phys. (2009) 130, 174713.
RESULTS: F+H2
Arrhenius plot of quantum, RPMD, and classical rate coefficients for the distinguishable atom H+H2 reaction between 200 and 1500 K (quantum results stopping at 1000 K).
Asymmetric barrier. Tc = 264 K.
R. Collepardo-Guevara, Yu. V. Suleimanov, and D. E. Manolopoulos, J. Chem. Phys. (2009) 130, 174713.
RESULTS: F+H2
R. Collepardo-Guevara, Yu. V. Suleimanov, and D. E. Manolopoulos, J. Chem. Phys. (2009) 130, 174713.
))(,())(,()( pQTSTRPMD qstqsTkTk κ⋅=
Asymmetric barrier. Tc = 264 K.
RESULTS: F+H2
R. Collepardo-Guevara, Yu. V. Suleimanov, and D. E. Manolopoulos, J. Chem. Phys. (2009) 130, 174713.
centroid formalism
))(,())(,()( pQTSTRPMD qstqsTkTk κ⋅=
Asymmetric barrier. Tc = 264 K.
Qualitative change in behaviour for iωb
→ ..TF
The deep tunnelling regime
.)(etc
RESULTS: F+H2
R. Collepardo-Guevara, Yu. V. Suleimanov, and D. E. Manolopoulos, J. Chem. Phys. (2009) 130, 174713.
centroid formalism
))(,())(,()( pQTSTRPMD qstqsTkTk κ⋅=
Asymmetric barrier. Tc = 264 K.
symm
asym
RESULTS: Mu+H2
Classical minimum energy path (blue solid line) and vibrationally adiabatic curve for the (000) state (red dashed line) for the Mu+H2 reaction vs. the natural reaction coordinate.
R. P. de Tudela*, F. J. Aoiz, Yu. V. Suleimanov*, and D. E. Manolopoulos, J. Phys. Chem. Lett. (2012) 3, 493–497. (* - equally contributed to this work)
Classical minimum energy path
vibrationally adiabatic curve for the (𝟎𝟎𝟎) state
RESULTS: Mu+H2
Classical minimum energy path (blue solid line) and vibrationally adiabatic curve for the (000) state (red dashed line) for the Mu+H2 reaction vs. the natural reaction coordinate.
R. P. de Tudela*, F. J. Aoiz, Yu. V. Suleimanov*, and D. E. Manolopoulos, J. Phys. Chem. Lett. (2012) 3, 493–497. (* - equally contributed to this work)
tunneling is suppressed
Classical minimum energy path
vibrationally adiabatic curve for the (𝟎𝟎𝟎) state
RESULTS: Mu+H2
Classical (dashed red line) and RPMD (blue solid line) potentials of mean force for the
Mu+H2 reaction at 1000 and 200 K.
Classical (red dashed line) and RPMD (blue solid line) transmission coefficients for the Mu+H2 reaction at
1000 and 200 K.
R. P. de Tudela*, F. J. Aoiz, Yu. V. Suleimanov*, and D. E. Manolopoulos, J. Phys. Chem. Lett. (2012) 3, 493–497. (* - equally contributed to this work)
RESULTS: Mu+H2
Arrhenius plot of QM, RPMD, classical and QCT rate coefficients for the Mu+H2 reaction between 200 and 1000 K.
R. P. de Tudela*, F. J. Aoiz, Yu. V. Suleimanov*, and D. E. Manolopoulos, J. Phys. Chem. Lett. (2012) 3, 493–497. (* - equally contributed to this work)
RESULTS: Mu+H2
R. P. de Tudela*, F. J. Aoiz, Yu. V. Suleimanov*, and D. E. Manolopoulos, J. Phys. Chem. Lett. (2012) 3, 493–497. (* - equally contributed to this work)
kRPMD(T) is:
• simple to compute • equal to kQTST(T) in the limit as t→0+ • bounded from above by kQTST(T) in the limit as t → ∞ • independent of s(q) in the limit as t → ∞ • reliable at high temperatures • captures the zero-point energy effect • within a factor of 2-3 of the exact QM results in the deep
quantum tunneling regime
→ complex chemical reactions!
RESULTS: H+CH4
s0(q)=0 s1(q)=0
;)(0 Rq −= ∞Rs { })(),(),(),(max)(1 rsrsrsrss δγβα=q
[ ] HHrHCr HHrHCrs
xx
xxx
)()( )()()(−−−−
−−−−=∗∗
r
Yu. V. Suleimanov, R. Collepardo-Guevara, and D. E. Manolopoulos, J. Chem. Phys. (2011) 134, 044131.
RESULTS: H+CH4
Classical (dashed) and RPMD (solid) potentials of mean force for the H+CH4 reaction at 1000 and 200 K.
Classical (dashed) and RPMD (solid) transmission coefficients for the H+CH4 reaction at 1000 and 200 K.
Yu. V. Suleimanov, R. Collepardo-Guevara, and D. E. Manolopoulos, J. Chem. Phys. (2011) 134, 044131.
RESULTS: H+CH4
Arrhenius plot of various approximate quantum mechanical rate coefficients for the H+CH4 reaction between 200 and 2000 K.
Asymmetric barrier. Tc = 296 K.
Yu. V. Suleimanov, R. Collepardo-Guevara, and D. E. Manolopoulos, J. Chem. Phys. (2011) 134, 044131.
RESULTS: H+CH4
Percentage deviation of the QI, centroid QTST, CVT/μOMT, and RPMD rate coefficients from the more accurate MCTDH results in the temperature range from 225 to 400 K.
Yu. V. Suleimanov, R. Collepardo-Guevara, and D. E. Manolopoulos, J. Chem. Phys. (2011) 134, 044131.
A+BC % error: • QI: ~10% • QTST: ~50% • CVT: ~10-15%
kRPMD(T) is:
• simple to compute • equal to kQTST(T) in the limit as t→0+ • bounded from above by kQTST(T) in the limit as t → ∞ • independent of s(q) in the limit as t → ∞ • reliable at high temperatures • captures the zero-point energy effect • within a factor of 2-3 of the exact QM results in the deep
quantum tunneling regime
→ complex chemical reactions!
3. RPMDrate
Comp. Phys. Comm., In Press (October 2012)
http://ysuleyma.scripts.mit.edu
Incorporated algorithms Bennett-Chandler factorization of the rate coefficient. [1] Bennett, C. H. In Algorithms for Chemical Computations, ACS Symposium Series No. 46; Christofferson, R. E., Ed.; American Chemical Society: Washington DC, 1977; p 63. [2] Chandler, D. Statistical mechanics of isomerization dynamics in liquids and the transition state approximation, J. Chem. Phys. 1978, 68, 2959. Umbrella integration along the reaction coordinate. [3] Kästner, J.; Thiel, W. Bridging the gap between thermodynamic integration and umbrella sampling provides a novel analysis method: “Umbrella integration” J. Chem. Phys. 2005, 123, 144104. [4] Kästner, J.; Thiel, W. Analysis of the statistical error in umbrella sampling simulations by umbrella integration J. Chem. Phys. 2006, 124, 234106. [5] Kästner, J. Umbrella integration in two or more reaction coordinates, J. Chem. Phys. 2009, 131, 034109. RATTLE algorithm for constrained molecular dynamics simulations. [6] Andersen, H. C. Rattle: A “velocity” version of the shake algorithm for molecular dynamics calculations, J. Comput. Phys. 1983, 52, 24. Andersen thermostat. [7] Andersen, H. C. Molecular dynamics simulations at constant pressure and/or temperature, J. Chem. Phys. 1980, 72, 2384. Colored-Noise, generalized Langevin equation thermostats. [8] Ceriotti, M.; Bussi, G.; Parrinello, M. Langevin equation with colored noise for constant-temperature molecular dynamics simulations, Phys. Rev. Lett. 2009, 102, 020601. [9] Ceriotti, M.; Bussi, G.; Parrinello, M. Nuclear quantum effects in solids using a colored-noise thermostat, Phys. Rev. Lett. 2009, 103, 030603. [10] Ceriotti, M.; Bussi, G.; Parrinello, M. Colored-noise thermostats a la carte, J. Chem. Theory Comput. 2010, 6, 1170. [11] Ceriotti, M.; Manolopoulos, D. E.; Parrinello, M. Accelerating the convergence of path integral dynamics with a generalized Langevin equation, J. Chem. Phys. 2011, 134, 084104.
3. RPMDrate
Example input file for the H + H2 reaction.
Yu. V. Suleimanov, J. W. Allen, and W. H. Green, Comp. Phys. Comm. 184 (2013) 833
Yu. V. Suleimanov, J. W. Allen, and W. H. Green, Comp. Phys. Comm. 184 (2013) 833
3. RPMDrate
Classical (solid) and centroid (dashed) potentials of mean force for the H + H2, H + CH4, OH + CH4, H + C2H6 reactions at 300 K.
Yu. V. Suleimanov, J. W. Allen, and W. H. Green, Comp. Phys. Comm. 184 (2013) 833
3. RPMDrate
Classical (solid) and RPMD (dashed) time-dependent transmission coefficients for the H + H2, H + CH4, OH + CH4, H + C2H6 reactions at 300 K.
Yu. V. Suleimanov, J. W. Allen, and W. H. Green, Comp. Phys. Comm. 184 (2013) 833
3. RPMDrate
Classical (solid) and RPMD (dashed) time-dependent transmission coefficients for the H + H2, H + CH4, OH + CH4, H + C2H6 reactions at 300 K.
Method k(T = 300 K), cm3molecule-1
s-1 RPMD 4.28(-17)
QI 1.15(-16)
CVT/SCT 1.44(-16)
Experiment 2.54(-17) (295 K)
• OH + HO2 • RPMDrate v2.0 • …
http://ysuleyma.scripts.mit.edu/ Yu. V. Suleimanov et al. CPC, 2013
RPMDrate
• Mu + H2 • H + H2 • D + H2 • Heμ + H2 • Cl + O3 • ….
Prof. F. Javier Aoiz Group Universidad Complutense
de Madrid
Prof. Hua Guo Group University of New Mexico
• Mu + CH4 • H + CH4 • O + CH4 • Cl + CH4 • OH + CO • ….
Dr. Albert F. Wagner Argonne National
Laboratory
Dr Yohann Scribano Universite de Montpellier
• Ion-molecule reactions (D+ + H2…)
• OH + HO2 • RPMDrate v2.0 • …
http://ysuleyma.scripts.mit.edu/ Yu. V. Suleimanov et al. CPC, 2013
RPMDrate
• Mu + H2 • H + H2 • D + H2 • Heμ + H2 • Cl + O3 • ….
Prof. F. Javier Aoiz Group Universidad Complutense
de Madrid
Prof. Hua Guo Group University of New Mexico
• Mu + CH4 • H + CH4 • O + CH4 • Cl + CH4 • OH + CO • ….
Dr. Albert F. Wagner Argonne National
Laboratory
Dr Yohann Scribano Universite de Montpellier
• Ion-molecule reactions (D+ + H2…)
• Joshua W. Allen • William H. Green
• Stephen Klippenstein • Albert Wagner • David Manolopoulos • Rosana Collepardo-
Guevara • Javier Aoiz • Ricardo Perez de Tudela
• Hua Guo