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

(
n
)

U

(
n
)

GL

(
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. cianfa72

    I ##SU(2, \mathbb C)## parametrization using Euler angles

    Hi, I found on some lectures the following parametrization of ##SU(2, \mathbb C)## group elements \begin{pmatrix} e^{i(\psi+\phi)/2}\cos{\frac{\theta}{2}}\ \ ie^{i(\psi-\phi)/2}\sin{\frac{\theta}{2}}\\ ie^{-i(\psi-\phi)/2}\sin{\frac{\theta}{2}}\ \ e^{-i(\psi+\phi)/2}\cos{\frac{\theta}{2}}...
  2. cianfa72

    I ##SU(2)## homeomorphic with ##\mathbb S^3##

    Hi, ##SU(2)## group as topological space is homeomorphic to the 3-sphere ##\mathbb S^3##. Since ##SU(2)## matrices are unitary there is a natural bijection between them and points on ##\mathbb S^3##. In order to define an homeomorphism a topology is needed on both spaces involved. ##\mathbb...
  3. spin_100

    A SU(2) and SU(3) representations to describe spin states

    Spin 1/2 particles are two states system in C^2 and so it is natural for the rotations to be described by SU(2), for three states systems like spin - 1 particle, Why do we still use SU(2) and not SU(3) to describe the rotations? Is it possible to derive them without resorting to the eigenvalue...
  4. graviton_10

    I Showing that operators follow SU(2) algebra

    For two quantum oscillators, I have raising and lowering operators and , and the number operator . I need to check if operators below follow commutation relations. Now as far as I know, SU(2) algebra commutation relation is [T_1, T_2] = i ε^ijk T_3. So, should I just get T_1 and T_2 in...
  5. James1238765

    I How Is the Matrix V Related to Dirac Spinors and Tensor Products?

    Could anyone help with some of the later parts of the derivation for Dirac spinors, please? I understand that an arbitrary vector ##\vec v## $$ \begin{bmatrix} x \\ y \\ z \end{bmatrix} $$ can be defined as an equivalent matrix V with the components $$ \begin{bmatrix} z & x - iy \\ x + iy...
  6. W

    B Why are SU(3), SU(2) and U(1) groups used in the Standard Model?

    hi, i have studied Standard Model for particle physics - at present it is described by three groups - i have studied - these groups but could not establish what particular feature suggest of these group to be used to describe SM. Thanks
  7. J

    Model with SU(2) gauge symmetry and SO(3) global symmetry

    1.) The rule for the global ##SO(3)## transformation of the gauge vector field is ##A^i_{\mu} \to \omega_{ij}A^j_{\mu}## for ##\omega \in SO(3)##. The proof is by direct calculation. First, if ##A^i_{\mu} \to \omega_{ij}A^j_{\mu}## then ##F^i_{\mu \nu} \to \omega_{ij}F^j_{\mu\nu}##, so...
  8. Ramtin123

    A Why Is the Mixed SU(2) Term Invariant in Scalar Multiplet Models?

    Consider two arbitrary scalar multiplets ##\Phi## and ##\Psi## invariant under ##SU(2)\times U(1)##. When writing the potential for this model, in addition to the usual terms like ##\Phi^\dagger \Phi + (\Phi^\dagger \Phi)^2##, I often see in the literature, less usual terms like: $$\Phi^\dagger...
  9. K

    I Ladder operators and SU(2) representation

    Hello! I read in many places the derivation of the representation for SU(2) using ladder operators and in all of the places they say that, due to the fact that we are looking for a finite dimensional representation, the ladder must end at a point, hence why we have an eigenvector of ##L_3##...
  10. P

    I Why choose traceless matrices as basis?

    While writing down the basis for SU(2), physicists often choose traceless hermitian matrices as such, often the Pauli matrices. Why is this? In particular why traceless, and why hermitian?
  11. JuanC97

    I SU(2) invariance implies isotropy?

    Hello guys, I've came up with three statements in a discussion with a friend where we were trying to check if we had a clear vision of what isotropy and group invariance would imply in an arbitrary theory of gravity at the level of its matter lagrangian. We got stuck at some point so I came here...
  12. S

    I Spin group SU(2) and SO(3)

    Hello! I want to make sure I understand the relation between this and rotation (mainly between SU(2) and SO(3), but also in general). Also, I am a physics major, so I apologize if my statements are not very rigorous, but I want to make sure I understand the basic underlying concepts. So SU(2) is...
  13. S

    I Understanding SU(2) and SO(3) Representations

    Hello! I am reading some representation theory and I am a bit confused about some stuff. I read that SU(2) is the double covering of SO(3), so to each matrix in SO(3) corresponds one in SU(2). I am not sure I understand this. So if we have a 3D representation of SU(2), the 3D object it acts on...
  14. N

    Adjoint representation of SU(2)

    Homework Statement [/B] I am looking at this document. http://www.math.columbia.edu/~woit/notes3.pdf Homework Equations [/B] ad(x)y = [x,y] Ad(X) = gXg-1The Attempt at a Solution [/B] I understand how ad(S1) and X is found but I don't understand what g and g-1 to use to find Ad(X). Also...
  15. fresh_42

    Insights A Journey to The Manifold SU(2) - Part II - Comments

    Greg Bernhardt submitted a new PF Insights post A Journey to The Manifold SU(2) - Part II Continue reading the Original PF Insights Post.
  16. fresh_42

    Insights A Journey to The Manifold - Part I - Comments

    fresh_42 submitted a new PF Insights post A Journey to The Manifold - Part I Continue reading the Original PF Insights Post.
  17. davidge

    I Irreducible representation of SU(2)

    I'm reading a paper on physics where it's said it can be shown that every irreducible representation of ##SU(2)## is equivalent to the one which uses the Ladder Operators. I am a noob when it comes to this subject, but I'd like to know whether or not the proof is easy to carry out.
  18. S

    I SU(2) Generators: Understanding Lie Algebra

    Hello! I am reading some Lie Algebra and at a point the author says that for a vector with 3 cartesian components ##V_i## i =1,2,3 the commutation relations with the generators of rotation are: ##[J_i,V_j]=i\epsilon_{ijk}V_k##. Can someone explain this to me? I am confused as ##V_j## is a number...
  19. T

    I Why does SU(2) have 3 parameters/generators like the SO(3)?

    From "Symmetry and the Standard Model: Mathematics and Particle Physics by Matthew Robinson", it states that 'SU(2) matrix has one of the real parameters fixed,leaving three real parameters'. I don't really get this part and hope someone can clear my doubt...
  20. G

    Invariance under SU(2) in quantum mechanics

    Homework Statement Hi, I'm trying to self-study quantum mechanics, with a special interest for the group-theoretical aspect of it. I found in the internet some lecture notes from Professor Woit that I fouund interesting, so I decided to use them as my guide. Unfortunately I'm now stuck at a...
  21. T

    I Standard Model SU(2) singlets and doublets

    I know that for SU(2), weak interaction, in the standard model the right handed leptons are singlets, (and right handed neutrinos don't exist). For right handed quarks are they singlets or doublets in the standard model. So is it (u d)R or is it just u(R) and d(R)
  22. Kara386

    Irreducible representation of su(2)

    Homework Statement Using the irreducible representation of ##su(2)##, with ##j=\frac{5}{2}##, calculate ##J_z##, ##exp(itJ_z)## and ##J_x##. Homework EquationsThe Attempt at a Solution There seem to be loads of irreducible representations of ##su(2)## online, but no reference at all to a...
  23. Safinaz

    I Commutation relation of hypercharge and SU(2) generators

    Hi all, I read in Cheng and Li's book "Gauge theory of elementary particle physics" Ch 11, specifically : Eq. (11.46) that the hypercharge commutes with the SU(2) generators, i.e., ##[Q-T_3,T_i]=0##, I'd like to understand what that mean and how this could be proved ?
  24. S

    I Unitary Matrix Representation for SU(2) Group: Derivation and Verification

    The matrix representation ##U## for the group ##SU(2)## is given by ##U = \begin{bmatrix} \alpha & -\beta^{*} \\ \beta & \alpha^{*} \\ \end{bmatrix}## where ##\alpha## and ##\beta## are complex numbers and ##|\alpha|^{2}+|\beta|^{2}=1##. This can be derived using the unitary of...
  25. S

    I Can Quarks Form a Basis for SU(2) Using Only the I3 Space?

    Hello! I am reading something related to algebra in particle physics and I want to make sure I got it. So, they say the u, d and s quarks can represent the basis of the SU(3) representation when the diagonalizable matrices are Y=B+S and ##I_3##. But, if I want to look only in the ##I_3## space...
  26. N

    I Understanding Weak Isospin in SU(2) Gauge Theory

    In QCD, quark is in fundamental representation of SU(3) and thus it has to have 3 charges (what we came to call "colors"). Gauge bosons are in adjoint representation and there are 8 of them. The choice how to assign color charges to them is not unique, one popular choice is based on Gell-Mann...
  27. S

    A Highest state of SU(2) algebra

    Let the generators of the SU(2) algebra be ##\tau_{1}##, ##\tau_{2}## and ##\tau_{3}##. Consider an ##N## dimensional representation, which means that the ##\tau_{i}## are ##N \times N## matrices which act on some ##N##-dimensional vector space. Consider the ladder operators...
  28. Glenn Rowe

    I Equivalence of SU(2) and O(3) in Ryder's QFT book

    I've got a question about the identification of SU(2) with O(3) in Ryder's QFT book (2nd edition) pages 34 - 35. The other posts on this topic I could find don't seem to address this question, so here goes. He derives the matrix in eqn 2.47: $$H= \left[\begin{array}{cc} -\xi_{1}\xi_{2} &...
  29. S

    I Understanding SU(2) Representations and Their Role in Particle Physics

    Hello! I just started reading about SU(2) (the book is Lie Algebras in Particle Physics by Howard Georgi) and I am confused about something - I attached a screenshot of those parts. So, for what I understood by now, the SU(2) are 2x2 matrices whose generators are Pauli matrices and they act on a...
  30. munirah

    Understanding the Parameters of SU(4) and SU(2)

    Homework Statement Good day, From my reading, SU(4) have 15 parameter and SU(2) has 3 paramater that range differently with certain parameter(rotation angle). And all the parameter is linearly independent to each other. My question are: 1. What the characteristic of each of the parameter? 2...
  31. M

    Isomorphism between so(3) and su(2)

    Homework Statement How do I use the commutation relations of su(2) and so(3) to construct a Lie-algebra isomorphism between these two algebras? Homework Equations The commutation relations are [ta, tb] = i epsilonabc tc, the ts being the basis elements of the algebras. They basically have the...
  32. A

    A Is SU(3) always contains SU(2) groups?

    Hi, I trying to understand. If there is non-trivial SU(3) group, is it always possible to find SU(2) as part of SU(3)? And same question about SU(2) and U(1).
  33. pellman

    I SU(2) and su(2) have different dimensions?

    The Lie group SU(2) is the set of unitary 2x2 matrices with determinant 1. These matrices can be written a b -b* a* Thus, as a manifold, we can think of a coordinate chart consisting of the four real numbers making up the two complex numbers a and b. It is a...
  34. C

    I Raising and lowering operators for a composite isospin SU(2)

    Consider pion states composed of ##q \bar q## pairs where ##q \in \left\{u,d \right\}## transforms under an ##SU(2)## isospin flavour symmetry. These bound states transform in the tensor product ##R_1 \otimes R_2## of two representations ##(R_1, R_2)## of ##SU(2)##. Take ##R_2## as the...
  35. B

    A SU(2)_V, SU(2)_A transformations

    Within my project thesis I stumbled over the term SU(2)_V, SU(2)_A transformations. Although I know U(1)_V, U(1)_A transformations from the left and right handed quarks( U(1)_V transformations transform left and right handed quarks the same way, while U(1)_A transformations transform them with a...
  36. terra

    SU(2) lepton doublet conjugation rules

    I have a left-handed ##SU(2)## lepton doublet: ## \ell_L = \begin{pmatrix} \psi_{\nu,L} \\ \psi_{e,L} \end{pmatrix}. ## I want to know its transformation properties under conjugation and similar 'basic' transformations: ##\ell^{\dagger}_L, \bar{\ell}_L, \ell^c_L, \bar{\ell}^c_L## and the general...
  37. ShayanJ

    Ryder's SU(2) Example in Quantum Field Theory

    In section 3.5 of his textbook Quantum Field Theory, Ryder discusses an example of a non-Abelian gauge theory. He considers a 3D internal space and rotations in this space. At first he shows that the fields in this internal space transform like ##\delta \vec \phi=-\vec \Lambda \times \vec \phi...
  38. Einj

    What combination of generators can produce a particular SU(2) matrix?

    Hello everyone, I have a question that will probably turn out to be trivial. I have the following matrix: $$ U=\text{diag}(e^{2i\alpha},e^{-i\alpha},e^{-i\alpha}). $$ This seems to me as an SU(2) matrix in the adjoint representation since it's unitary and has determinant 1. Am I right? If so...
  39. C

    Constructing states in SU(2)

    Homework Statement Construct the decompositions ##\mathbf 2 \otimes \mathbf 2 = \mathbf 3 \oplus \mathbf 1##, where ##\mathbf N## is the representation of su(2) with ##\mathbf N## states and thus spin j=1/2 (N-1). Homework Equations Substates within a state labelled by j can take on values -j...
  40. Meditations

    Additional Phase factors in SU(2)

    I am curious as to the meaning of, and name given to the phase ##\xi(t)## which may be added as a prefix to the time evolution operator ##\hat{U}(t)##. This phase acts to shift the energy of the dynamical phase ##<{\psi(t)}|\hat{H}(t)|\psi(t)>##, since it appears in the Hamiltonian along the...
  41. H

    SU(2) Rotation & Spinors: Connected?

    Hi, a fairly quick question. I'm reading Bruce Schumm's book "Deep Down Things" and he says that in SU(2) you have to rotate by 720 degrees to return to your starting point. This is clearly the same definition as a spinor. My question is, then, does rotation in SU(2) automatically imply the...
  42. Anchovy

    Weak interaction SU(2) gauge fields W^{1,2,3} and charge?

    When we start by postulating local SU(2) gauge invariance for our weak isospin doublets \begin{align} \psi &= \begin{pmatrix} \nu_{e} \\ e^{-} \end{pmatrix}_{L} \end{align} etc., we have to introduce massless gauge fields to preserve the Lagrangian's invariance. For SU(2) this demands 3...
  43. N

    Is Weak Isospin Conservation Provable Using Noether's Theorem?

    Is it possible to prove that weak isospin associated with SU(2) is conserved using Noether's theorem?
  44. S

    What is the general form of the rotation matrix in SU(2) space?

    Hi. I know that the \sigma matrices are the generators of the rotations in su(2) space. They satisfy [\sigma_i,\sigma_j]=2i\epsilon_{ijk}\sigma_k It is conventional therefore to take J_i=\frac{1}{2}\sigma_i such that [J_i,J_j]=i\epsilon_{ijk}\sigma_k . Isn't there a problem by taking these...
  45. topsquark

    MHB SU(2) and elementary properites of Lie Algebras

    I've been having fun with my new Lie Algebra text and it occurred to me that working out a couple of basic examples of my own would be a good idea. I got rather large surprise. The example I'm working with is SU(2) and I'm going through some basic properties it has. For all its uses in...
  46. I

    SU(2): Get RHS from LHS of Expression

    Please, I'm stuck. How to get the rhs from the lhs? X^{\alpha}_{\ \ \alpha^{\ \prime}}X^{\beta}_{\ \ \beta^{\ \prime}}\epsilon^{\alpha^{\ \prime}\beta^{\ \prime}}=det X\epsilon^{\alpha\beta}
  47. K

    SU(3) defining representation (3) decomposition under SU(2) x U(1) subgroup.

    I have been reading Georgi "Lie Algebras in Particle Physics" and on page 183 he mentions how that the SU(3) defining representation decomposes into an SU(2) doublet with hyperchage (1/3) and singlet with hypercharge (-2/3). I am confused on how he knows this. I apologize if this is not the...
  48. TrickyDicky

    SU(2) as a normal subgroup of SL(2, C)

    SU(2) matrices act isometrically on the Riemann sphere with the chordal metric. At the same time the group of automorphisms of the Riemann sphere is isomorphic to the group SL(2, C) of isometries of H 3(hyperbolic space) i.e. every orientation-preserving isometry of H 3 gives rise to a Möbius...
  49. H

    Connection between SU(2) and SO(3)

    I am somewhat confused with the connection between the two groups. In the text I'm reading (An Introduction to Tensors and Group theory for physicists N. Jeevanjee), there is a chapter quite early on (in the group theory part) which outlines a homomorphism from SU(2) to SO(3), however I find...
  50. TrickyDicky

    Is SU(2) the key to understanding quantum numbers and symmetry?

    Is it purely coincidental that the internal symmetry related flavor quantum numbers(like isospin and weak isospin) and the spacetime symmetry related spin quantum number have SU(2) as underlying group? They refer to seemingly unrelated things but it is remarkable how ubiquitous SU(2) is.
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