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Published equation contexts

ρR(g)=UR(g)ρR(e)UR(g)†\rho_R(g)=U_R(g)\rho_R(e)U_R(g)^\dagger

Why this formula appears here

Choose a declared laboratory frame L only as a temporary coordinate system. Let gRLg_{RL} be the rotor’s orientation relative to L . A covariant family of rotor states can be written ρR(g)=UR(g)ρR(e)UR(g)†\rho_R(g)=U_R(g)\rho_R(e)U_R(g)^\dagger. This is a definition. e is the identity orientation, URU_R is a unitary representation of G , and ρR(e)\rho_R(e) is the chosen fiducial state. Nothing in the equation makes g absolute. Changing the reference frame by h changes the coordinate label and representation together.

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Published contexts (1)

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ρR(g)=UR(g)ρR(e)UR(g)†.\rho_R(g)=U_R(g)\rho_R(e)U_R(g)^\dagger.

Equation 17 · Evolutionary Physics

A Reference Frame Becomes Classical by Publishing Its Orientation

This equation states an equality: the expressions on both sides have the same value under the article’s assumptions.

Choose a declared laboratory frame L only as a temporary coordinate system. Let gRLg_{RL} be the rotor’s orientation relative to L . A covariant family of rotor states can be written ρR(g)=UR(g)ρR(e)UR(g)†\rho_R(g)=U_R(g)\rho_R(e)U_R(g)^\dagger. This is a definition. e is the identity orientation, URU_R is a unitary representation of G , and ρR(e)\rho_R(e) is the chosen fiducial state. Nothing in the equation makes g absolute. Changing the reference frame by h changes the coordinate label and representation together.

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