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SYMMETRIES in PHYSICS

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Symmetry and Spontaneous Symmetry Break<strong>in</strong>g<br />

Selected Groups and Symmetries<br />

Spontaneous Symmetry Break<strong>in</strong>g<br />

Fundamental Symmetries of Nuclear Forces [1]<br />

Denote ˆx df . = {⃗r,⃗p,⃗s,⃗t}. Nuclear <strong>in</strong>teractions have the form<br />

̂V (ˆx 1 , ˆx 2 ) ≡ ̂V C (ˆx 1 , ˆx 2 ) + ̂V T (ˆx 1 , ˆx 2 ) + ̂V LS (ˆx 1 , ˆx 2 ) + ̂V LL 2(ˆx 1 , ˆx 2 )<br />

where: C-central, T -tensor, LS-sp<strong>in</strong>-orbit and LL 2 -quadratic LS<br />

Central Interaction (r 12 ≡ |⃗r 1 −⃗r 2 |)<br />

̂V C (ˆx 1 , ˆx 2 ) = V 0 (r 12 ) + V s (r 12 ) [⃗s (1) · ⃗s (2) ]<br />

+ V t (r 12 ) [⃗t (1) ·⃗t (2) ]<br />

+ V s−t (r 12 ) [⃗s (1) · ⃗s (2) ] [⃗t (1) ·⃗t (2) ]<br />

Invariant under rotations, translations, <strong>in</strong>version and time-reversal<br />

Jerzy DUDEK<br />

<strong>SYMMETRIES</strong> <strong>in</strong> <strong>PHYSICS</strong>

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