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  2. Pauli matrices - Wikipedia

    en.wikipedia.org/wiki/Pauli_matrices

    The fact that the Pauli matrices, along with the identity matrix I, form an orthogonal basis for the Hilbert space of all 2 × 2 complex matrices , over , means that we can express any 2 × 2 complex matrix M as = + where c is a complex number, and a is a 3-component, complex vector.

  3. Spinors in three dimensions - Wikipedia

    en.wikipedia.org/wiki/Spinors_in_three_dimensions

    Given a unit vector in 3 dimensions, for example (a, b, c), one takes a dot product with the Pauli spin matrices to obtain a spin matrix for spin in the direction of the unit vector. The eigenvectors of that spin matrix are the spinors for spin-1/2 oriented in the direction given by the vector. Example: u = (0.8, -0.6, 0) is a unit vector ...

  4. Walsh function - Wikipedia

    en.wikipedia.org/wiki/Walsh_function

    Each Rademacher operator acts on one particular fermion coordinate only, and there it is a Pauli matrix. It may be identified with the observable measuring spin component of that fermion along one of the axes {,,} in spin space. Thus, a Walsh operator measures the spin of a subset of fermions, each along its own axis.

  5. Pauli group - Wikipedia

    en.wikipedia.org/wiki/Pauli_group

    The Pauli group is generated by the Pauli matrices, and like them it is named after Wolfgang Pauli. The Pauli group on n {\displaystyle n} qubits, G n {\displaystyle G_{n}} , is the group generated by the operators described above applied to each of n {\displaystyle n} qubits in the tensor product Hilbert space ( C 2 ) ⊗ n {\displaystyle ...

  6. Yang–Mills equations - Wikipedia

    en.wikipedia.org/wiki/Yang–Mills_equations

    The dx 1 ⊗σ 3 coefficient of a BPST instanton on the (x 1,x 2)-slice of R 4 where σ 3 is the third Pauli matrix (top left). The dx 2 ⊗σ 3 coefficient (top right). These coefficients determine the restriction of the BPST instanton A with g=2, ρ=1,z=0 to this slice. The corresponding field strength centered around z=0 (bottom left).

  7. Gauge theory (mathematics) - Wikipedia

    en.wikipedia.org/wiki/Gauge_theory_(mathematics)

    The dx 1 ⊗σ 3 coefficient of a BPST instanton on the (x 1,x 2)-slice of R 4 where σ 3 is the third Pauli matrix (top left). The dx 2 ⊗σ 3 coefficient (top right). These coefficients determine the restriction of the BPST instanton A with g=2,ρ=1,z=0 to this slice. The corresponding field strength centered around z=0 (bottom left).

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    www.aol.com/games/play/masque-publishing/simply...

    Simply Jigsaw. Piece together a new jigsaw puzzle every day, complete with themes that follow the seasons and a super useful edges-only tool. ... World Class Poker. Play. Masque Publishing. In ...

  9. Talk:Pauli matrices - Wikipedia

    en.wikipedia.org/wiki/Talk:Pauli_matrices

    The notation employed, and explained clearly for the Pauli vector, is universal in the physics community, and often detailed in most textbooks. The quantity in the parenthesis is a matrix. The quantity in the parenthesis is a matrix.

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