What is Su(2): Definition and 120 Discussions

In mathematics, the special unitary group of degree n, denoted SU(n), is the Lie group of n × n unitary matrices with determinant 1.
The more general unitary matrices may have complex determinants with absolute value 1, rather than real 1 in the special case.
The group operation is matrix multiplication. The special unitary group is a subgroup of the unitary group U(n), consisting of all n×n unitary matrices. As a compact classical group, U(n) is the group that preserves the standard inner product on





C


n




{\displaystyle \mathbb {C} ^{n}}
. It is itself a subgroup of the general linear group,



SU

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n
)

U

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n
)

GL

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n
,

C

)


{\displaystyle \operatorname {SU} (n)\subset \operatorname {U} (n)\subset \operatorname {GL} (n,\mathbb {C} )}
.
The SU(n) groups find wide application in the Standard Model of particle physics, especially SU(2) in the electroweak interaction and SU(3) in quantum chromodynamics.The simplest case, SU(1), is the trivial group, having only a single element. The group SU(2) is isomorphic to the group of quaternions of norm 1, and is thus diffeomorphic to the 3-sphere. Since unit quaternions can be used to represent rotations in 3-dimensional space (up to sign), there is a surjective homomorphism from SU(2) to the rotation group SO(3) whose kernel is {+I, −I}. SU(2) is also identical to one of the symmetry groups of spinors, Spin(3), that enables a spinor presentation of rotations.

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  1. D

    SU(2) Spinor: Is Product of Two Scalar-Type Entity?

    I'm having a memory blank on this particular area of field theory. Is the product of two spinors a scalar or scalar type entity and if so, can I treat it like a scalar? (i.e. move it around without worrying about order etc) i.e. is \Phi_1^{\dagger} \Phi_1 a scalar? and if so does...
  2. M

    Infinite dimensional representation of su(2)

    I'm trying to understand this paper which the author claimed that he had constructed an infinite dimensional representation of the su(2) algebra. The hermitian generators are given by J_x=\frac{i}{2}(\sqrt{N+1}a-a^\dagger\sqrt{N+1} ) J_y=-\frac{i}{2}(\sqrt{N+1}a+a^\dagger\sqrt{N+1} )...
  3. C

    Connection between the SU(2) group for the spin 1/2

    I wanted to ask if there is any connection between the SU(2) group for the spin 1/2 and the gauge group of weak interactions. I feel there isn't much of a connection other than the fact that they share the same group properties, but I am not sure. Thanks to anyone in advance that can clarify...
  4. I

    Study Lie Groups: G. 't Hooft's SU(2) Index Convention

    I'm studying Lie groups using G. 't Hooft's tutorial: http://www.phys.uu.nl/~thooft/lectures/lieg.html In page 34, he introduces superscript and subscript indices starting from equation 6.27: \phi_{\alpha} \rightarrow \phi_{\alpha}' = X_{\beta}^{\alpha}\phi^{\beta} What is the...
  5. S

    Su(2) Lie Algebra in SO(3): Why Choose Omega/2?

    hi ,i see from a book su(2) has the form U\left(\hat{n},\omega\right)=1cos\frac{\omega}{2}-i\sigmasin\frac{\omega}{2} in getting the relation with so(3),why we choose \frac{\omega}{2},how about changing for \omega? thank you
  6. diegzumillo

    Show that Isospin operators satisfy the SU(2) algebra

    Hi there! Doesn't seem like a hard problem.. Homework Statement Show that the 3 isospin operators, defined by T_{+}\left\vert p\right\rangle =0, T_{-}\left\vert n\right\rangle =0, T_{+}\left\vert n\right\rangle =\left\vert p\right\rangle, T_{-}\left\vert p\right\rangle =\left\vert...
  7. Jim Kata

    How Is the Center of SU(2) Related to the Fundamental Group of SO(3)?

    there's a surjective homomorphism from a : SU(2) --> SO(3) The kernel of this homomorphism is the center of SU(2) which is Z/2Z. Now the fundamental group of SO(3) is Z/2Z. This is a general thing. The simplest version of my question is how is the center of SU(2) related to the...
  8. C

    Structure constants of su(2) and so(3)

    SU(2) and SO(3) "have the same Lie algebra". While I understand that their corresponding lie algebras su(3) and so(2) have the same commutator relations \mbox{SO(3)}: \left[ \tau^i, \tau^j\right] = \iota \varepsilon_{ijk} \tau^k \mbox{SU(2)}: \left[ \frac{\sigma^i}{2}...
  9. J

    Motivation for SU(2) x U(1) and charge operator

    I've read that the choice of Gauge group \mathrm{SU}(2)_\mathrm{L}\times \mathrm{U}(1)_\mathrm{Y} can be justified by the fact that the electromagnetic charge and the flavour-changing weak charge do not form a closed SU(2) current algebra. The solution is to tack on an additional U(1) group and...
  10. J

    What are weight spaces and how do they relate to the representation of SU(2)?

    I'm taking a course on Lie groups and am reading alongisde Cahn's semi-simple lie algebras and their representations. On page 4 he starts to construct a representation T of the Lie group corresponding to SU(2) acting on a linear space V, by defining the action of T_z and T_+ on a vector v_j...
  11. U

    SU(2) Rotation Representation: Why ω/2?

    Any rotation about n(θ, φ) in SU(2) can be represent as u(n, ω) = I cos[ω/2] - i(σ.n)sin[ω/2],where I is the unit matrix and i is the complex number.Right? But can someone tell me why ω/2 rather than ω? Waiting for your response.Thank you.
  12. P

    Spin/ angular momentum, representations of SO(3), SU(2)

    Homework Statement I'm trying to understand why particles have both spin and angular momentum in terms of group theory. As I understand it orbital angular momentum comes from the normal generators SO(3) which are intuitively infintesimal rotations so d/d(theta) etc. Also spin comes from...
  13. P

    Exploring Connections Between Spin, SO(3), and SU(2)

    I’ve got a couple of conceptual questions on spin etc, and any help would be appreciated. First of all reading books (eg. Sakuri) it seems like authors tend to show there’s a homomorphism between the groups SO(3) and SU(2) using Euler angles etc. I know the Pauli matricies act as generators...
  14. P

    Spin: why su(2) for an electron

    Sorry if this is a silly question (I'm doing a fairly basic QM course but am doing a bit of extra reading for interest etc.), but why for an spin hbar/2 particle is the spin operators (the Pauli matricies) the generator of su(2)? I understand why generally generators act as conserved...
  15. A

    Representations of SU(2) are equivalent to their duals

    Hi. I am having trouble proving that the irreducible representations of SU(2) are equivalent to their dual representations. The reps I am looking at are the spaces of homogenous polynomials in 2 complex variables of degree 2j (where j is 0, 1/2, 1,...). If f is such a polynomial the action of...
  16. C

    Trying to understand spin networks, or at least SU(2)

    Hi. I'm a relative layman with a CS/Math background (with more of the former than the latter) and I've been trying to follow some of the recent developments in physics with a hope of eventually understanding at least the outline of the underlying math. I had a couple of questions about some...
  17. E

    SO(10) -> SU(3) x SU(2) x U(1) -inflation?

    I'm trying to learn some theory of inflation, and recently read a paper by Andrei Linde from 1982 where he suggested a scenario where inflation is driven by the phase transition SU(5) -> SU(3) x SU(2) x U(1). Now SU(5) is known to not be a good candidate as an extension of the standard model...
  18. kakarukeys

    Finite Dimensional Representation of SU(2)

    Does anybody know whether the following irreducible representations of SU(2) are unitary? g belongs to SU(2) [U_j(g) f](v) = f(g^{-1} v) f is an order-2j homogeneous complex polynomial of two complex variables v = (x, y) e.g. for j = 1, f = 2x^2 + 3xy + 4y^2
  19. marcus

    Complexifying su(2) to get sl(2,C)-group thread footnote

    Complexifying su(2) to get sl(2,C)---group thread footnote On the group thread midterm exam (which we never had to take!) it says what is the LA of the matrix group SL(2, C) and the answer is the TRACE ZERO 2x2 matrices. So that is what sl(2,C) is. When you exponentiate one of the little...
  20. marcus

    Question about irred rep of SU(2) that factor by the covering map

    Let φ SU(2) ---> SO(3) be the double covering Any irreducible representation of SO(3) pulls back by φ to provide an irreducible representation of SU(2) on the same finite dimensional Hilbert space. this seems clear, almost not worth saying: the pullback is obviously irred. and...
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