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Consider that the density of states g(E) for super relativistic gas is defined as [1, 0 ED g(E)= The specific heat at constant volume

Consider that the density of states g(E) for super relativistic gas is defined as [1, 0 ED g(E)= The specific heat at constant volume Cy for gas of bosons and fermions in very low temperature limit (T 0) varies as O Cy a T for bosons and Cy a T for fermions O Ca I for bosons and Cy a T for fermions O Cya T for bosons and C a T for fermions O Ca T for bosons and Cy a T for fermions

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