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Zero-point Energy Leakage in Quantum Thermal Bath Molecular Dynamics Simulations Fabien Brieuc, Yael Bronstein, Hichem Dammak, Philippe Depondt, Fabio Finocchi, and Marc Hayoun J. Chem. Theory Comput., Just Accepted Manuscript • DOI: 10.1021/acs.jctc.6b00684 • Publication Date (Web): 21 Oct 2016 Downloaded from http://pubs.acs.org on October 24, 2016
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Journal of Chemical Theory and Computation is published by the American Chemical Society. 1155 Sixteenth Street N.W., Washington, DC 20036 Published by American Chemical Society. Copyright © American Chemical Society. However, no copyright claim is made to original U.S. Government works, or works produced by employees of any Commonwealth realm Crown government in the course of their duties.
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Journal of Chemical Theory and Computation
† § ‡ § ∗ † ¶ ‡
∗ ‡ ¶
! "# $ % & '
! $ ( ) *+ ,,- !
! " # $%&' ! #! ( !
!! " # $ ‡ %& ' ( ) *"!"! $ ¶ ' + , -. //!0 $ § , 1 ∗
†
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! ! ) $%&' ! $%&' ! * + # , " $%&' , - #
$%&' , * ) ) ! ! *
!
" # $ % # # &' ' # # #
(
# # $ ) ) *
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Journal of Chemical Theory and Computation
# #
+ # , - # ) # ./ 0 ! ./
,
$ # # ./) # 1 ) 2 3 # # $ ./ # 2 1
4 ./ 5) 2
6&7- 2 # "
6&7- 2 # ) ) " 6&7- # ! - ) 8
9 ./ 6&7- #
# / ) 5 2 $ 6&7- ./ 2 # 4 6&7- # ./) # / ) 5 2 # # $ )
2 2 : 2
6&7- 2 #
$ 6&7- ./) ;
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# ./ < 6&7- 3 # ./ 1 = ) - )8 / %3 '
./ # , - ! / - ./ x m # f (x) =
m¨ x = f (x) − mγ x˙ + R(t)
) # # R(t) # : 5 =
< R(t) > = 0 < R(t)R(t + τ ) > =
* +∞ −∞
IR (ω, T ) −iωτ
ω . 2π
;
7 ; ()>
&4 IR (ω, T ) T # ?
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Journal of Chemical Theory and Computation
&4 &4 Ix # < ) =
χ˜ (ω) =
ω Ix (ω, T ) 2kB T
?
˜ (ω) # χ(ω) ˜ 1 χ ˜ x ˜(ω) 1 R(ω) =
˜ x˜(ω) = χ(ω) ˜ R(ω)
@
1 # # &4 Ix &4 IR = 2 Ix (ω, T ) = |χ(ω)| ˜ IR (ω, T )
A
< ) # =
2kB T χ˜ (ω) IR (ω, T ) = . 2 ω |χ(ω)| ˜ ' ω0
B
@
#
χ(ω) ˜ =
m [ω02
1 . − ω 2 + iγω]
C
/ B &4 # =
IR (ω, T ) = 2mγ kB T
∀ω.
/ ()> ;
D
- # ' @
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# kB T ω ' # #
⎤
⎡
1 1 ⎦ θ(ω, T ) = ω ⎣ + 2 exp ω − 1 kB T
E
./ &4 D # # E # < ) # F ( # > # =
χ ˜ (ω) =
ω Ix (ω, T ) 2θ(ω, T )
()> &4 R(t) ./ =
IR (ω, T ) = 2mγ θ(ω, T )
*
' - IR ω R(t) # # )! ω # ) ./ = 0 γ )! ω # ( - 0 γ # , # # / +
ω # # ) A
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Journal of Chemical Theory and Computation
ω γ ' 2 # ω 2ω ω # ' ./) 0 γ D *
' # ./) ) 2 # ./) ) 4G # # $
H= 1 1 1 1 H = mx˙ 21 + mω12 x21 + mx˙ 22 + mω22 x22 + C3 (x1 − x2 )3 + C4 (x1 − x2 )4 2 2 2 2
;
x1 x2 ω1 ω2 ) m C3 C4 $ H #
˜ = H/ω1 = H 2 2 2 2 ˜ = q˙1 + q1 + q˙2 + Ω2 q2 + c3 (q1 − q2 )3 + c4 (q1 − q2 )4 H 2 2 2 2
?
# =
ω2 Ω= , ω1
ξ=
, mω1
xi qi = , ξ
C3 ξ 3 c3 = , ω1
C4 ξ 4 c4 = , ω1
t∗ = ω1 t,
q˙i =
dqi . @ dt∗
q1 q2 Ω ω1 > ω2 ) # B
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Ω=0.5
0.5 0.4 0.3 0.2 0
2
4
6
8 104 x c3
0.6 average energy
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
average energy
Journal of Chemical Theory and Computation
10
12
14
Ω=0.25
0.4 0.2 0 0
5
10
QTB
15
20 4 10 x c4
QTB
ε1
25
30
QTB
ε2
εc
35
Exact
1 = 1 2 c # ./) c3 c4 = # c3 = 0 c4 = 0 Ω = 0.5 - = c4 = 0 c3 = 0 Ω = 0.25 / c = 0 # 6&7- ./ ' < # 1 2 =
1 =
q˙12 2
+
q12 2
,
2 =
q˙22 2
2
+Ω
q22 2
.
A
./) 0 γ = 4 × 10−4 ω1
)! ω = 2ω1 δt = 0.05ω1−1 ;E " 107 Ω EE@HEC c3 c4 EH25 × 10−4 EH40 × 10−4 , kB T = 0.03 ω1 T ∼ 60 > ω1 = 2π × 40 $5 # # 5) C
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1 0.8
ζ
(a)
4
10 x c3 = 2.4 9.7 14.6 19.4
0.6 0.4 0.2 0 0.48
0.5
0.52
0.54
0.56
0.58
0.6
Ω 1
0.6
ζ
(b)
104 x c4 = 3.9 7.7 15.4 30.8
0.8
0.4 0.2 0 0.1
0.2
0.3
0.4
0.5
0.6
0.7
0.8
Ω
1 *= 6) 2 , ζ B
Ω @ = # c3 = 0 c4 = 0 - = c4 = 0 c3 = 0 5) 9 1 = 0.5 2 = Ω/2 1
# ./ =
Ω = 0.5 # Ω = 0.25 c3 = 0 c4 = 0 ./ 5) ' c3 c4 ./) =
* 6&7-
' 6&7- Ω c3 c4 , $ 1 ζ 6&7-=
Δ − Δ ( − ) − ( − ) 1 2 1 2 ζ= = Δ 1 − 2
B
( , 2 ζ = 1 D
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-4
(a)
arbitrary units 0
ω1-ω2
2ω2
0.5
1
γ=4x10 ω1
ω1+ω2
1.5
2
0
-4
(b)
-3
(c)
γ=4x10 ω1
0.5
1
2 -3
(d)
γ=4x10 ω1
1.5
γ=4x10 ω1
arbitrary units
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
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0
0.5
1
1.5
2
0
0.5
ω/ω1 oscillator 1
1
ω/ω1
1.5
2
oscillator 2
1 ;= I# * # # ./) # Ω = 0.5 c3 = 2.4 × 10−4
Ω = 0.2 c4 = 15.4 × 10−4 0= γ = 4 × 10−4 ω1 γ = 4 × 10−3 ω1
= = ' 2 ζ = 0 1 2 1,2 = 1,2 ' , * # ζ Ω !
c3 c4 % 6&7- Ω ' # Ω = 0.5 , * ' # 2 # # # 2ω , # # ./) # , ; = 2ω2 ω1 − ω2 ω1 + ω2 # Ω = 0.5 # (ω1 ; 2ω2) (ω2 ; ω1 − ω2 ) 4 # 3ω 9 6&7 # Ω = 1/3 , *# ( , 6&7- Ω 1 ;# Ω = 0.2 c4 = 15.4 × 10−4 ω1 ω2 E
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Ω=0.5
0.5
2x10-2 1x10-2
0.4
4x10
-3
4x10
-4
4x10-3
0.3
1x10-2 -2 2x10
0
average energy
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Journal of Chemical Theory and Computation
average energy
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2
4
6
8 4 10 x c3
10
12
14
Ω=0.25
0.5 0.4 0.3 0.2 0.1 0
5
10
15
20 4 10 x c4
25
30
35
1 ?= 7! 0 γ ω1 A = # c3 = 0 c4 = 0 Ω = 0.5 - = c4 = 0 c3 = 0 Ω = 0.25 # # ./) $ 2 , 6&7- Ω < 1/3 γ
0
4 × 10−4 ω1 2 × 10−2 ω1 ( 6&7- = Ω = 0.5 # Ω = 0.25 , * 1 ? 6&7- γ ' γ 2 # ' c3 = 2.4 × 10−4
γ 4 × 10−3 ω1 0 6&7- ζ = 0.08 1 ; # # γ = 6&7- # 2 2ω2 ω1 − ω2 ω1 + ω2 # 6&7- γ # 2
γ/2π -
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γ 6&7- , ? 1 ; γ
Ω = 0.2 c4 = 15.5 × 10−4 0 # ! ' ttr # JI7
ttr
# # * 1 @ ttr Ω = 0.5 # c3 6&7- γ ω = 1/ttr 1
c3 = 4 × 10−4 , ttr ∼ 400ω1−1 ω ∼ 2.5 × 10−3ω1 , ? γ = 10−2 ω1 2 6&7- γ ω Ω=0.5 1500
-1
ttr (ω1 )
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
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1000
500 1
1.5
2
2.5
3
3.5
4
-4
10 x c3
1 @= 7 # ttr ω1−1 # c3 Ω = 0.5 JI7 $ c4 = 0 ' =
# , ! 6&7- # γ # # ( *
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Journal of Chemical Theory and Computation
( ) 3 3 # #
# # % %H$ ) # 8 )# =
V (r) =
−b(r−r0 )
a(r−r0 ) u0 a e − 1 + b e − 1 − u0 a + bea(r−r0 )
C
r %H$ u0 # r0 # %H$ a b = r0 = 0.96 K # %$− a 7.11 K−1
b 2.00 K−1 u0 = 2.73 I %H$ ν
V 100 $5 % %H% # # =
2 V (R) = C0 1 − e−α0 (R−R0 ) − C0
D
C0 α0 R0 %H% # = C0 = 3.81 I R0 = 2.88 K
α0 %H% ν # 10 60 $5 ./) 0.1 # # * " 3 # V (r) + V (R − r)
#) ( , L L %H$ # ∼ 1 K
L # L ∼ 1.9 K 5 # %)$ ;
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! 6&7- )# ) ν2 %H% ) ν1 %H$ ' %H$
) %H% ' < Ω = ν2 /ν1 0 γ 6&7- T = 600 >
ν2 α0 D ν , 100 $5 ν1 ./) &' # P = 20 1 ./) 2 2
# &' ' 2 2 , ) ) ! T T $ % , 2 = N 1 kB T (i) = E 2 N i=1 k
N 1 (i) kB T = E , 2 N i=1 k
*E
(i)
N = 3 N = 3 # $ % Ek
2 i ' 2 # = ! = ) 2 ! ./ &' 1 , A 2 !
?
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2500 effective temperature (K)
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Journal of Chemical Theory and Computation
H - PIMD ZPEL
2000
H - QTB-MD O - QTB-MD
ZPEL
1500
O - PIMD
1000 0
1000
2000 time (ps)
3000
4000
1 A= 7! T T ./) &' T = 600K $ Ω = 0.5 γ = 0.2 $5 6&7- ' 6&7- # , =
ζ=
(T − T )() − (T − T )() (T − T )()
.
*
ζ = 0 2 0 < ζ < 1 2 Ω , B 4 3 ; 6&7- Ω ∼ 1/2 1 B 6&7- # # # γ % 6&7- # Ω < 0.2= ! Ω
1 C #
d d Ω = 0.5 ./) &' ) ' , C d # ! # 6&7- % d # 6&7-= ./) # # 2 6&7- $ 6&7- # @
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1
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γ = 0.2 THz γ = 2 THz γ = 5 THz γ = 10 THz γ = 20 THz
0.8 0.6 ζ
0.4 0.2 0 0.2
0.3
0.4
0.5
0.6
0.7
Ω
1 B= 6&7- , # ζ , *
Ω γ ./) d # &'
(
γ # 9 2 # 2 γ , ; 1 D # ) Ω = 0.5 ! γ 0.2 10 $5 1 γ = 0.2 $5 6&7- γ = 10 $5 6&7 , B ( 0 # 2 $ 2 , # γ 7 # #
' ! 2 # # 6&7- 6&7- # # F 0 6&7- ' 9 A
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(a) : = 0.5
-1
probability density (Å )
2 Standard-MD PIMD
1.5
QTB-MD (0.2 THz) QTB-MD (20 THz)
1 0.5 0 0.8
1 d
1.2
OH
-1
10
1.4
(Å)
12 probability density (Å )
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Journal of Chemical Theory and Computation
: = 0.5
(b)
8 6 4 2 0 2.7
2.8 d
2.9 (Å)
3
3.1
OO
1 C= &# # # %H$ %H% # ) &' ./) 0 γ 0.2 20 $5 Ω = 0.5 # # #
( ! 0 γ 6&7-
M ./) / ) N5 . 6&7- T = 10 > # - )8 /kB = 1450.6 > σ = 2.54 K ! = 1.37σ = 3.49 K ' ) ) # ./ # B
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Journal of Chemical Theory and Computation
0.7
γ=2 THz γ=10 THz
0.6 0.5 arbitrary units
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
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0.4 0.3 0.2 0.1 0 20
40
60
80
100
120
frequency (THz)
1 D= I# # # ./) Ω = 0.5 0= γ = 0.2 $5 # γ = 10 $5 # 2 ( ./) 1
! γ ( , γ = 0.9 $5 ./) # # , E ' # # # $ γ E $5 # ./) # θ(ν, T )
E #
, E 6&7- 5 # ./ , E # 5 # # γ 0 6&7- γ = 9 $5 1 γ 2 # # # ./) ./ - # # # 2 # ) %4 1 γ γ Δω 2 %4 γ , # F
γ # # Δν = Δω/2π = γ/2π C
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J = 0.9 THz J = 10 THz
200
150 1
slope / QD slope
K
B
2 E /k (K)
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Journal of Chemical Theory and Computation
100
50
0.8 0.6 0.4 0.2 0
0
2
0
4
2
4
6
6
J (THz)
8
10
8
frequency (THz)
1 E= 4 2 # T = 10 > # ./) γ ED E $5 )! 20 $5 # . θ(ν, T ) E ν = ω/2π '= γ # 5 # ,
' - %4
# # 5 1 #
kB T ' ./) kB T # # θ(ω, T ) E 1
6&7- %4 # ./) " ) ' ,
# 6&7-
%4 # # ./) " # ) )
/ %3 /% 5 # ! # < ' ) ) = # + # % # F 7 ,
D
ACS Paragon Plus Environment
Journal of Chemical Theory and Computation
(a)
Standard-MD (10 THz) QTB-MD (10 THz)
(b)
Standard-MD (2 THz) QTB-MD (2 THz)
DOS (ps)
500 400 300 200 100 0
500
DOS (ps)
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Page 20 of 40
400 300 200 100 0
0
5
10
15
20
frequency (THz)
1 = I# %4 ! γ # 1 ) 5 # kB T - # θ(ν, T ) E ./) 0 γ = 10 $5
# 2 $5
*E
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Page 21 of 40
5 4 # ./ #
./)
> *BE >
- # / /% # ! $ ,) ) $ 0 γ E@ A $5 )! ν @ $5 $ γ ) +)% %) )F 1 *
0.03
reduced polarization
1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23 24 25 26 27 28 29 30 31 32 33 34 35 36 37 38 39 40 41 42 43 44 45 46 47 48 49 50 51 52 53 54 55 56 57 58 59 60
Journal of Chemical Theory and Computation
PIMD QTB (16 THz)
0.02 R
C
C
200
T O
T (K)
0.01
T
O
300
100
R 0
0 100
1
J(THz)
150
200
10
250
300
T (K)
1 *= 5 ) / %3 # # ./) γ = 16 $5 &' P = 16 I # +)% %) )F 0 γ ./ 5 # # &' 5 # # ./)
γ = 16 $5 1 ./) = +)%))F &'
# P = 16 = AE >
DE > *@@ > # # &' A; >
DC > *@C >
, *
γ ./) 1 γ # # *
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Journal of Chemical Theory and Computation
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Page 22 of 40
' γ ./ = ! 6&7- #
( 5) 2 6&7- ./) # ./ ! ( 6&7- # # # $ γ , 2 2 # /% # # ./ ! # ./
# < ) ./ ) ) 6&7- ) ) = # # # # ./ ' # ./ # # γ # # ! #
$ !
6&7- ./) γ -
**
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Journal of Chemical Theory and Computation
) F ! # # , # ./) # # 2 # ' # ./) # # γ γ # 2 %)$ # )# γ % # # ! # ./ 0 0 6&7- # ' ./ = #
# 2 # ./)
( 2 # 2 # :O : /% # ( 2 8 )- / -8 # P/ 2 , F +O 3Q) )1 ' % 2 $&F LOL F 4 O # F 4 O FJ+4
*;
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Page 24 of 40
< + # # # 2
. #
# . , $ : R(t) =
R(t) = 0 R(t)R(t + τ ) =
** +∞
−∞
IR (ω, T )−iωτ
ω 2π
*;
()> R(t) IR (ω, T ) ' ./) IR # * tn = nδt : # # : # Xj Wj +∞
Rn ≡ R(tn ) =
*?
Wj Xj+n
j=−∞
# Xj 5 1 *; *? Wj # =
+∞
Wj Wj−l =
j=−∞
+∞ −∞
IR (ω, T )−iωtl
ω 2π
*@
˜ (ω) , 1 W (t)= tl = lδt W Wj ≡ W (tj ) =
+∞
−∞
*?
˜ (ω)−iωtj ω W 2π
ACS Paragon Plus Environment
*A
Page 25 of 40
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Journal of Chemical Theory and Computation
M *A δt → 0= +∞
Wj Wj−l
j=−∞
∞
˜ (ω)W ˜ (−ω)−iωtl ω W 2π −∞
1 = δt
*B
˜ (ω) # F W (t) W *@ *B=
˜ (ω) = W
=
√ Wj = δt
δtIR (ω, T )
ω IR (ω, T )−iωtj 2π
+∞
−∞
*C
*D
' 5 1
1 Wj = √ N 1 Xj = √ N
N/2
˜ l −i2πjl/N W
;E
˜ l −i2πjl/N X
;
l=−N/2+1 N/2 l=−N/2+1
N # / *D ;E=
1 Wj = √ Nδω
+∞ −∞
˜ (ω)−iωtj ω W
;*
Nδtδω = 2π #
˜l = √ 1 W Nδt ωl = lδω 1 ;E ;
Rn =
IR (ωl )
;;
˜ −l X ˜ l −i2πnl/N W
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Rn N/2 l=−N/2+1
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;; Rn , = N/2 1 ˜ l −i2πnl/N Rn = √ IR (ωl )X Nδt l=−N/2+1
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˜ l - , 1 R 1 Rn = √ N
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;B
˜ l # : # X ˜ + iN ˜l ˜ l = Ml √ X 2
;C
˜ l N ˜l : # 5 M ˜ l M ˜l = M ˜ −l # X ˜l = −N˜−l 1 = N ˜l = R
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!" #
- # , /% - )# # # # . &# # ' ) 2 # i m - # =
dpi i − pG pi − 1 . T r(pG ) pi = fi − γpi + R dt Wg Nf Wg
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; × ; 2γG Wg kB T # 5 δt # *B
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