Le cours de physique (18 blocs) :
mécanique quantique (7) et physique statistique (11)
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+ CD-rom d’illustrations et de simulations, Manuel Joffre
Outils pour le cours de mécanique quantique
Livres (existent aussi en anglais) :
•! « Mécanique quantique »
•! « Problèmes quantiques » Jean-Louis Basdevant et Jean Dalibard
Chaque semaine: un QCM à remplir à l’adresse :
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Idées clés de la description quantique d'un système physique :
Principes de la mécanique quantique
!! Etats du système
!! "Observables" de ce système
!! Evolution dans le temps du système
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1.
Quand a-t-on besoin de la mécanique quantique ?
action = longueur impulsion Particule ponctuelle de masse
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(non relativiste)Physique newtonienne ou physique ondulatoire ?
Les concepts classiques cessent de s'appliquer quand : action caractéristique < constante de Planck
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':''W%&'#.0)!"%4)&'''''''%"''''''''-#$$4"%1"='e1'.%4"'.)0.!)%)'(!'.!)"+-4(%'7!1&' 41'0"!"'#t'(J+$.4(&+#1'&%(#1':'%"'(J+$.4(&+#1'&%(#1'F'"'&+$4("!10$%1"''
@+%1'70>+1+%&':'
! ψ | A ˆ
2| ψ " = a
2α(1)
! ψ | A ˆ | ψ " = a
α(2)
| ψ " (3)
A ˆ (4)
B ˆ (5)
A ˆ B ˆ = ˆ B A ˆ (6)
[ ˆ A, B] ˆ ≡ A ˆ B ˆ − B ˆ A ˆ (7)
[ ˆ A, B] = 0 ˆ (8)
| ψ
i" (9)
α
iβ
i(10)
ˆ p
x= ¯ h
i
∂
∂x (11)
ψ(x, y, z) = e
ikxxφ(y, z) (12)
‘
¯
hk
x(13)
ˆ p
y= ¯ h
i
∂
∂y (14)
ψ(x, y, z) = e
ikyyχ(x, z) (15)
ψ(x, y, z) = e
ikxxe
ikyyF (z) (16)
! ψ | A ˆ
2| ψ " = a
2α(1)
! ψ | A ˆ | ψ " = a
α(2)
| ψ " (3)
A ˆ (4)
B ˆ (5)
A ˆ B ˆ = ˆ B A ˆ (6)
[ ˆ A, B] ˆ ≡ A ˆ B ˆ − B ˆ A ˆ (7)
[ ˆ A, B] = 0 ˆ (8)
| ψ
i" (9)
α
iβ
i(10)
ˆ p
x= ¯ h
i
∂
∂x (11)
ψ(x, y, z) = e
ikxxφ(y, z) (12)
‘
¯
hk
x(13)
ˆ p
y= ¯ h
i
∂
∂y (14)
ψ(x, y, z) = e
ikyyχ(x, z) (15)
ψ(x, y, z) = e
ikxxe
ikyyF (z) (16)
! ψ | A ˆ
2| ψ " = a
2α(1)
! ψ | A ˆ | ψ " = a
α(2)
| ψ " (3)
A ˆ (4)
B ˆ (5)
A ˆ B ˆ = ˆ B A ˆ (6)
[ ˆ A, B] ˆ ≡ A ˆ B ˆ − B ˆ A ˆ (7)
[ ˆ A, B] = 0 ˆ (8)
| ψ
i" (9)
α
iβ
i(10)
ˆ p
x= ¯ h
i
∂
∂x (11)
ψ(x, y, z) = e
ikxxφ(y, z) (12)
‘
¯
hk
x(13)
ˆ p
y= ¯ h
i
∂
∂y (14)
ψ(x, y, z) = e
ikyyχ(x, z) (15)
ψ(x, y, z) = e
ikxxe
ikyyF (z) (16)
MM:N'
:%
c/%$.(%'F:'-#$$%1"'"+)%)'.!)"+'7J41%'&6$0")+%'r'
*#4K%$%1"'7!1&'41'.#"%1"+%('.!+)'
!K%-'
e1'+1")#74+"'(J#.0)!"%4)'8.!)+"09''''''70>+1+'.!)' W!'&6$0")+%'7%'(J5!$+("#1+%1'&%'")!74+"'.!)':'
[!(%4)&'.)#.)%&':'
c"!"&'.)#.)%&:'>#1-"+#1&'.!+)%&'#4'+$.!+)%&' e1'.%4"'-5%)-5%)'(%&'0"!"&'.)#.)%&'7%'''''''
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%"'''''''#1"'7#1-'41%'@!&%'7%'>#1-"+#1&'.)#.)%&'-#$$41%&'
H
ˆ (1)
Etot.
= ¯
h2K22M +
Erel.(2)
−
¯
h22µ
∆ψ("r) +
V("
r)ψ("
r) =
Erel.ψ("
r) (3)
H
ˆ
rel.ψ =
Erel.ψ (4)
Ψ(R,
" "
r) =
eiK!·R!ψ("
r) (5)
¯
h2K22M (6)
eiK
"
·R" (7)
Φ("re,
"
rp) = ψ(
R," "
r) (8)
[ ˆ
Hc.m.,Hˆ
rel.] = 0 (9)
[ˆ
x,pˆ
x] =
i¯h(10)
[ ˆ
X,Pˆ
x] =
i¯h(11)
" ˆ
R, P
" ˆ (12)
" ˆ
r,"
pˆ (13)
µ
=
mpmemp
+
me(14)
H
ˆ
rel.=
pˆ
22µ +
V(ˆ "
r)(15)
M
=
mp+
me(16)
H
ˆ
c.m.=
Pˆ
22M (17)
H
ˆ = ˆ
Hc.m.+ ˆ
Hrel.(18)
P
ˆ (1)
H
ˆ (2)
Etot.
= ¯
h2K22M +
Erel.(3)
−
¯
h22µ
∆ψ("r) +
V("
r)ψ("
r) =
Erel.ψ("
r) (4)
H
ˆ
rel.ψ =
Erel.ψ (5)
Ψ(R,
" "
r) =
eiK·! R!ψ("
r) (6)
¯
h2K22M (7)
eiK
"
·R" (8)
Φ("re,
"
rp) = ψ(
R," "
r) (9)
[ ˆ
Hc.m.,Hˆ
rel.] = 0 (10)
[ˆ
x,pˆ
x] =
i¯h(11)
[ ˆ
X,Pˆ
x] =
i¯h(12)
" ˆ
R, P
" ˆ (13)
" ˆ
r,
"
pˆ (14)
µ
=
mpmemp
+
me(15)
H
ˆ
rel.=
pˆ
22µ +
V(ˆ "
r)(16)
M
=
mp+
me(17)
H
ˆ
c.m.=
Pˆ
22M (18)
H
ˆ = ˆ
Hc.m.+ ˆ
Hrel.(19)
! ψ | A ˆ
2| ψ " = a
2α(1)
! ψ | A ˆ | ψ " = a
α(2)
| ψ " (3)
A ˆ (4)
B ˆ (5)
A ˆ B ˆ = ˆ B A ˆ (6)
[ ˆ A, B] ˆ ≡ A ˆ B ˆ − B ˆ A ˆ (7)
[ ˆ A, B] = 0 ˆ (8)
[ ˆ A, B] ˆ % = 0 (9)
| ψ
i" (10)
α
iβ
i(11)
ˆ p
x= ¯ h
i
∂
∂x (12)
ψ(x, y, z) = e
ikxxφ(y, z) (13)
‘
¯
hk
x(14)
ˆ p
y= ¯ h
i
∂
∂y (15)
ψ(x, y, z) = e
ikyyχ(x, z) (16)
ψ(x, y, z) = e
ikxxe
ikyyF (z) (17)
ˆ
p
x(18)
e@&%)K!@(%&'34+'1%'-#$$4"%1"'.!&'
P+'7%4/'#@&%)K!@(%&'1%'-#$$4"%1"'.!&Z'-J%&"aXa7+)%'&+'''''''''''''''''''''''Z' +('1J%&"'%1'2010)!('.!&'.#&&+@(%'7%'.)0.!)%)'(%'&6&",$%'7!1&'41'0"!"'#t'' (%&'34!1"+"0&'
A
'%"'B
'"'@+%1'70"%)$+10%&=''A(4&'.)0-+&0$%1"':'
! ψ | A ˆ
2| ψ " = a
2α(1)
! ψ | A ˆ | ψ " = a
α(2)
| ψ " (3)
A ˆ (4)
B ˆ (5)
A ˆ B ˆ = ˆ B A ˆ (6)
[ ˆ A, B] ˆ ≡ A ˆ B ˆ − B ˆ A ˆ (7)
[ ˆ A, B] = 0 ˆ (8)
[ ˆ A, B] ˆ % = 0 (9)
| ψ
i" (10)
α
iβ
i(11)
ˆ p
x= ¯ h
i
∂
∂x (12)
ψ(x, y, z) = e
ikxxφ(y, z) (13)
‘
¯
hk
x(14)
ˆ p
y= ¯ h
i
∂
∂y (15)
ψ(x, y, z) = e
ikyyχ(x, z) (16)
ψ(x, y, z) = e
ikxxe
ikyyF (z) (17)
ˆ
p
x(18)
∆a ∆b ≥ 1 2
! !
!! ψ | [ ˆ A, B] ˆ | ψ " ! ! !
->='AI'(19)
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4".#'8*&'$.%"*:%@$8#$*.,%4.-4.$,%!$%%
A#4)'41'&6&",$%'+&#(0Z''''''''%&"'+170.%17!1"'74'"%$.&'
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l!'#@"%1+)'(%'K%-"%4)''''''''''''''X''1V+$.#)"%'34%('+1&"!1"'4("0)+%4)'2)z-%'X':' M'''''''+170.7"='74'"%$.&N'
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!K%-'
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!(#)&' n=1
n=2
n=0
∆a∆b≥ 1 2
!!
!"ψ|[ ˆA,B]ˆ|ψ#!!! (19)
ψ0(x)∝e−x2/2a2 (20)
∆a∆b≥ 1 2
!!
!"ψ|[ ˆA,B]ˆ|ψ#!
!! (19)
ψ0(x)∝e−x2/2a2 (20)
ψ1(x)∝x e−x2/2a2 (21)
∆a ∆b ≥ 1 2
! !
!" ψ | [ ˆ A, B] ˆ | ψ # ! ! ! (19)
ψ
0(x) ∝ e
−x2/2a2(20)
ψ
1(x) ∝ x e
−x2/2a2(21)
a = "
¯
h/mω (22)
(E
1− E
0)/¯ h = ω (23)
" x # (t) = a
√ 2 cos(ωt) (24)
ω (25)
∆a∆b≥ 1 2
!!
!"ψ|[ ˆA,B]ˆ|ψ#!
!! (19)
ψ0(x)∝e−x2/2a2 (20)
ψ1(x)∝x e−x2/2a2 (21)
a="
¯
h/mω (22)
(E1−E0)/¯h=ω (23)
"x#(t) = a
√2 cos(ωt) (24)
ω (25)
Aˆ (26)
¯
hω (27)
!(#)&'
*#74(!"+#1'7%''''''''''''''''''''X'(!'.4(&!"+#1'
∆a∆b≥ 1 2
!!
!"ψ|[ ˆA,B]ˆ|ψ#!
!! (19)
ψ
0(x)∝e−x2/2a2 (20)ψ
1(x)∝x e−x2/2a2 (21)a="
¯
h/mω (22)
(E1−E0)/¯h=
ω
(23)A!)'%/%$.(%':' P+'(V0"!"'+1+"+!('%&"'
!x"(t) =x0 cos(ωt) (1)
!ψ|Aˆ2|ψ"=a2α (2)
!ψ|Aˆ|ψ"=aα (3)
|ψ" (4)
Aˆ (5)
Bˆ (6)
AˆBˆ = ˆBAˆ (7)
[ ˆA,B]ˆ ≡ AˆBˆ−BˆAˆ (8)
[ ˆA,B] = 0ˆ (9)
[ ˆA,B]ˆ %= 0 (10)
|ψi" (11)
αi βi (12)
ˆ px= ¯h
i
∂
∂x (13)
ψ(x, y, z) =eikxxφ(y, z) (14)
‘
¯
hkx (15)
ˆ py= ¯h
i
∂
∂y (16)
ψ(x, y, z) =eikyyχ(x, z) (17)
ψ(x, y, z) =eikxxeikyyF(z) (18)
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A
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