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Q3mini

Guides

  • Fermionic Quantum Computation
  • Q3: Symbolic Quantum Simulation
  • Quantum Information Systems
  • Quantum Many-Body Systems
  • Quantum Spin Systems

Tech Notes

  • About Q3
  • Q3: Quick Start
  • Quantum Fourier Transform
  • Quantum Information Systems with Q3
  • Quantum Many-Body Systems with Q3
  • Quantum Operations
  • Quantum Spin Systems with Q3
  • Quantum States
  • Quantum Teleportation
  • Quick Quantum Computing with Q3

Symbols

  • Basis
  • Boson
  • Bra
  • CNOT
  • ControlledGate
  • ExpressionFor
  • Fermion
  • Heisenberg
  • Ket
  • Let
  • Majorana
  • Matrix
  • Multiply
  • NambuGreen
  • NambuHermitian
  • NambuMatrix
  • NambuUnitary
  • Pauli
  • Phase
  • QuantumCircuit
  • Qubit
  • Qudit
  • RandomWickCircuitSimulate
  • Rotation
  • Species
  • Spin
  • SWAP
  • WickCircuit
  • WickEntanglementEntropy
  • WickEntropy
  • WickGreenFunction
  • WickJump
  • WickLindbladSolve
  • WickLogarithmicNegativity
  • WickMeasurement
  • WickMonitor
  • WickMutualInformation
  • WickNonunitary
  • WickSimulate
  • WickState
  • WickUnitary

Overviews

  • The Postulates of Quantum Mechanics
  • Quantum Algorithms
  • Quantum Computation: Models
  • Quantum Computation: Overview
  • Quantum Error-Correction Codes
  • Quantum Information Theory
  • Quantum Noise and Decoherence
QuantumMob`Q3mini`
Boson
​
Boson
represents Bosonic annihilation operators.
​
​
Let
[Boson,a,b,...]or
Let
[Boson,{a,b,...}]
declares
a
,
b
, ... to be bosonic operators.
​
Details and Options

Examples  
(2)
Basic Examples  
(1)
Bosons are declared as follows
In[1]:=
Let[Boson,a,b]
By the above declaration, a[i,j,...] are all bosonic annihilation operators, and Dagger[a[i,j,...]] are creation operators.
This form is equivalent to the above form.
In[2]:=
a[2]**a[1]​​Dagger[a[1]]**a[2]​​a[i]**Dagger[a[j]]
Out[2]=
a
2
a
1
Out[2]=
†
a
1
a
2
Out[2]=
δ
i,j
+
†
a
j
a
i
The defining properties of bosonic operators are the canonical commutation relations
In[3]:=
a[1]**Dagger[a[1]]-Dagger[a[1]]**a[1]1​​a[1]**a[1]-a[1]**a[1]0​​Dagger[a[1]]**Dagger[a[1]]-Dagger[a[1]]**Dagger[a[1]]0
Out[3]=
True
Out[3]=
True
Out[3]=
True
These commutators can be conveniently assessed by Commutator[ ] and Anticommutator[ ]
In[4]:=
a[i]**Dagger[a[j]]**a[k]​​Commutator[a[i],Dagger[a[j]]]
Out[4]=
a
k
δ
i,j
+
†
a
j
a
k
a
i
Out[4]=
δ
i,j
Note that operators with different Heads are assumed to be different, regardless of their Flavor indices:
In[5]:=
a[i]**Dagger[b[j]]​​Commutator[a[i],Dagger[b[j]]]
Out[5]=
†
b
j
a
i
Out[5]=
0
Scope  
(1)

SeeAlso
Fermion
 
▪
Majorana
 
▪
Heisenberg
TechNotes
▪
Quantum Many-Body Systems with Q3
▪
Quantum Information Systems with Q3
▪
Quantum Spin Systems with Q3
▪
Q3: Quick Start
RelatedGuides
▪
Q3: Symbolic Quantum Simulation
▪
Quantum Many-Body Systems
▪
Quantum Information Systems
▪
Quantum Spin Systems
RelatedLinks
▪
Mahn-Soo Choi (2022)
, A Quantum Computation Workbook (Springer).
""

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