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Student Seminar: Classical and Quantum Integrable Systems

Student Seminar: Classical and Quantum Integrable Systems

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• Pseudo-orthogonal groups SO(p, q). Let g will be pseudo-Euclidean metric in<br />

the space R n p,q with p + q = n. The group SO(p, q) is the group of real matrices<br />

which preserve the form g:<br />

AgA t = g , detA = 1 .<br />

• Unitary group U(n) – the group of unitary n × n matrices:<br />

UU † = I .<br />

• Special unitary group SU(n) – the group of unitary n × n matrices with the<br />

unit determinant<br />

UU † = I , detU = 1 .<br />

• Pseudo-unitary group U(p, q):<br />

AgA † = g ,<br />

where g is the pseudo-Euclidean metric. Special pseudo-unitary group requires<br />

in addition the unit determinant detA = 1.<br />

• Symplectic group Sp(2n, R) or Sp(2n, C) is a group or real or complex matrices<br />

satisfying the condition<br />

AJA t = J<br />

where J is 2n × 2n matrix<br />

<strong>and</strong> I is n × n unit matrix.<br />

J =<br />

( ) 0 I<br />

−I 0<br />

Question to the class: What are the eigenvalues of J? Answer:<br />

J = diag(i, · · · i; −i, · · · , −i).<br />

Thus, the group Sp(2n) is really different from SO(2n)!<br />

The powerful tool in the theory of Lie groups are the Lie algebras. Let us see how<br />

they arise by using as an example SO(3). Let A be “close” to the identity matrix<br />

A = I + ɛa<br />

is an orthogonal matrix A t = A −1 . Therefore,<br />

I + ɛa t = (I + ɛa) −1 = I − ɛa + ɛ 2 a 2 + · · ·<br />

– 82 –

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