How Many States Exist Between E and E+δE in a Spin 1/2 System?

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SUMMARY

The discussion focuses on calculating the total number of states, denoted as Ω(E), within the energy range between E and E+δE for a system of N weakly interacting spin 1/2 particles. The energy of the system is defined by the equation E = -(n1-n2)μH, where n1 and n2 represent the number of spins aligned parallel and antiparallel to the magnetic field H, respectively. Participants suggest that since δE is significantly larger than μH, the summation of states can be approximated by an integral, drawing parallels to the classical "drunken sailor" problem to conceptualize the movement of particles within the energy range.

PREREQUISITES
  • Understanding of spin 1/2 systems and magnetic moments
  • Familiarity with statistical mechanics concepts
  • Knowledge of energy states and their calculations
  • Basic calculus for integral approximations
NEXT STEPS
  • Explore the derivation of the partition function for spin systems
  • Study the application of the Boltzmann distribution in statistical mechanics
  • Learn about the classical "drunken sailor" problem and its implications in physics
  • Investigate the concept of density of states in quantum mechanics
USEFUL FOR

Students and researchers in physics, particularly those studying statistical mechanics and quantum systems, will benefit from this discussion as it provides insights into calculating energy states in spin systems.

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Homework Statement


Consider an isolated system consisting of a large number N of very weakly interacting localized particles of spin 1/2. Each particle has a magnetic moment \mu which can point either parallel or antiparallel to an applied field H. The energy E of the system is then E = -(n1-n2)\muH, where n1 is the number of spins aligned parallel to H, and n2 is the number of spins aligned antiparallel to H.

(a) Consider the energy range between E and E+\deltaE where \delta is very small compared to E, but is microscopically large so that \deltaE>>\muH What is the total number of states \Omega(E) lying in this energy range?


Homework Equations


I really have no clue.


The Attempt at a Solution


I've been sitting with my small study group talking about this for an hour, and we're no closer to a solution than when we started. We've looked at the answer and it reminds us of the classical "drunken sailor" problem. Trust me when I say we've attempted this solution from every angle we can think of.
 
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How many states are there with a given/fixed energy, say, 0 or mu_H or mu*H or whatever it is?

After you know that, you'll want to sum up that number for every energy between E and delta E. Since the gap is big enough (delta E >> mu H), you can transform the sum into an integral.
 
Think about the possible number of states that exist between E and delta E. Like your drunken sailor problem, in which different ways could they move? How is that similar to your particles? Could you use a common formula for this situation as you might have used in the drunken sailor?
 

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