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PhyslibAlpha.Relativity.PauliMatrices.Anticommuting

Three anticommuting matrices are the most `2 × 2` can hold

i. Overview

A family `τ` of `2 × 2` complex matrices is anticommuting when `τ_a τ_b + τ_b τ_a = 2 δ_ab 1`: each `τ_a` squares to `1` and two different ones anticommute. Conjugating `τ_a` by another member reverses its sign, so every member is traceless, and the trace pairs the members with each other and with `1` orthonormally. Together with `1` they are linearly independent in the four dimensional space of `2 × 2` matrices, so such a family has at most three members. The Pauli matrices `σ1, σ2, σ3` attain the bound: they are a maximal anticommuting family, one for each axis of space.

ii. Key results

  • `IsAnticommuting` : the relation `τ_a τ_b + τ_b τ_a = 2 δ_ab 1`.
  • `IsAnticommuting.trace_mul`, `IsAnticommuting.trace_eq_zero` : the trace pairing.
  • `IsAnticommuting.linearIndependent` : the members together with `1` are independent.
  • `IsAnticommuting.card_le_three` : an anticommuting family has at most three members.
  • `isAnticommuting_pauliMatrix` : the Pauli matrices are anticommuting.
  • `isGreatest_card_isAnticommuting` : the largest anticommuting family has three members.

iii. Table of contents

  • A. Anticommuting families
  • B. At most three members
  • C. The Pauli matrices attain the bound

iv. References

* W. Pauli, *Zur Quantenmechanik des magnetischen Elektrons*, Z. Phys. 43 (1927) 601–623.

A. Anticommuting families

B. At most three members

C. The Pauli matrices attain the bound

9 declarations

definition

Anticommuting family of 2×22 \times 2 matrices τaτb+τbτa=2δabI\tau_a \tau_b + \tau_b \tau_a = 2 \delta_{ab} I

Let ι\iota be an index set. A family of 2×22 \times 2 complex matrices τ:ι→Mat(2,C)\tau: \iota \to \text{Mat}(2, \mathbb{C}) is said to be anticommuting if for all a,b∈ιa, b \in \iota, the relation τaτb+τbτa=2δabI\tau_a \tau_b + \tau_b \tau_a = 2 \delta_{ab} I holds, where II is the 2×22 \times 2 identity matrix and δab\delta_{ab} is the Kronecker delta (equal to 11 if a=ba = b and 00 otherwise). This implies that each matrix in the family squares to the identity (τa2=I\tau_a^2 = I) and any two distinct matrices anticommute (τaτb=−τbτa\tau_a \tau_b = -\tau_b \tau_a).

theorem

τa2=I\tau_a^2 = I for Anticommuting Families of 2×22 \times 2 Matrices

Let ι\iota be an index set and τ:ι→Mat(2,C)\tau: \iota \to \text{Mat}(2, \mathbb{C}) be an anticommuting family of 2×22 \times 2 complex matrices. For any a∈ιa \in \iota, the square of the matrix τa\tau_a is the identity matrix II, i.e., τa2=I\tau_a^2 = I.

theorem

τbτa=−τaτb\tau_b \tau_a = -\tau_a \tau_b for a≠ba \neq b

Let τ:ι→Mat(2,C)\tau: \iota \to \text{Mat}(2, \mathbb{C}) be an anticommuting family of 2×22 \times 2 matrices, which by definition satisfies τaτb+τbτa=2δabI\tau_a \tau_b + \tau_b \tau_a = 2 \delta_{ab} I for all a,b∈ιa, b \in \iota. For any two distinct indices a,b∈ιa, b \in \iota (where a≠ba \neq b), the matrices satisfy the anticommutation relation τbτa=−(τaτb)\tau_b \tau_a = -(\tau_a \tau_b).

theorem

tr(τaτb)=2δab\text{tr}(\tau_a \tau_b) = 2 \delta_{ab} for an Anticommuting Family of 2×22 \times 2 Matrices

For an anticommuting family of 2×22 \times 2 complex matrices τ\tau indexed by ι\iota, the trace of the product of any two matrices τa\tau_a and τb\tau_b is given by tr(τaτb)=2δab\text{tr}(\tau_a \tau_b) = 2\delta_{ab} where δab\delta_{ab} is the Kronecker delta (equal to 11 if a=ba = b and 00 otherwise). This means the trace is 22 when a=ba = b and 00 when a≠ba \neq b.

theorem

Distinct indices in an anticommuting family imply tr(τa)=0\text{tr}(\tau_a) = 0

Let {τk}k∈ι\{\tau_k\}_{k \in \iota} be an anticommuting family of 2×22 \times 2 complex matrices satisfying the relation τaτb+τbτa=2δabI\tau_a \tau_b + \tau_b \tau_a = 2 \delta_{ab} I for all a,b∈ιa, b \in \iota. If there exist two distinct indices a,b∈ιa, b \in \iota such that a≠ba \neq b, then the trace of the matrix τa\tau_a is zero (tr(τa)=0\text{tr}(\tau_a) = 0).

theorem

An anticommuting family of 2×22 \times 2 matrices and the identity are linearly independent

Let ι\iota be a finite index set with at least two elements. Let {τa}a∈ι\{\tau_a\}_{a \in \iota} be an anticommuting family of 2×22 \times 2 complex matrices such that τaτb+τbτa=2δabI\tau_a \tau_b + \tau_b \tau_a = 2 \delta_{ab} I for all a,b∈ιa, b \in \iota, where II is the 2×22 \times 2 identity matrix and δab\delta_{ab} is the Kronecker delta. Then the set of matrices {I}∪{τa}a∈ι\{I\} \cup \{\tau_a\}_{a \in \iota} is linearly independent over C\mathbb{C}.

theorem

An anticommuting family of 2×22 \times 2 matrices has cardinality at most 3

Let ι\iota be a finite index set and {τi}i∈ι\{\tau_i\}_{i \in \iota} be a family of 2×22 \times 2 complex matrices such that they satisfy the anticommutation relation τaτb+τbτa=2δabI\tau_a \tau_b + \tau_b \tau_a = 2 \delta_{ab} I for all a,b∈ιa, b \in \iota, where II is the identity matrix and δab\delta_{ab} is the Kronecker delta. Then the number of elements in the family is at most 3, i.e., ∣ι∣≤3|\iota| \leq 3.

theorem

The Pauli matrices σ1,σ2,σ3\sigma_1, \sigma_2, \sigma_3 form an anticommuting family

The family of Pauli matrices σ1,σ2,σ3\sigma_1, \sigma_2, \sigma_3 is anticommuting. That is, for any indices a,b∈{1,2,3}a, b \in \{1, 2, 3\}, the matrices satisfy the relation σaσb+σbσa=2δabI\sigma_a \sigma_b + \sigma_b \sigma_a = 2 \delta_{ab} I where II is the 2×22 \times 2 identity matrix and δab\delta_{ab} is the Kronecker delta. This implies that each Pauli matrix squares to the identity (σa2=I\sigma_a^2 = I) and any two distinct Pauli matrices anticommute (σaσb=−σbσa\sigma_a \sigma_b = -\sigma_b \sigma_a).

theorem

The maximum size of an anticommuting family of 2×22 \times 2 matrices is 3

The maximum size of an anticommuting family of 2×22 \times 2 complex matrices is 3. More precisely, let SS be the set of natural numbers nn such that there exists a family of nn matrices {τa}a=1n∈Mat(2,C)\{\tau_a\}_{a=1}^n \in \text{Mat}(2, \mathbb{C}) satisfying the anticommutation relation τaτb+τbτa=2δabI\tau_a \tau_b + \tau_b \tau_a = 2 \delta_{ab} I for all a,b∈{1,…,n}a, b \in \{1, \dots, n\}, where II is the 2×22 \times 2 identity matrix and δab\delta_{ab} is the Kronecker delta. Then 3 is the greatest element of SS. This implies that while the three Pauli matrices σ1,σ2,σ3\sigma_1, \sigma_2, \sigma_3 form such a family, no family of four or more such matrices exists.