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The neutron comprises multiple charged quarks. Can a particle that is electrically neutral but really composed of charged constituents have a magnetic dipole moment? Explain your answer.

Short Answer

Expert verified

Yes, an electrically neutral particle composed of charged constituents has a magnetic dipole moment.

Step by step solution

01

Explanation.

Each proton and each neutron contain three quarks. A quark is a fast-moving point of energy. There are several varieties of quarks. Protons and neutrons are composed of two types: up quarks and down quarks.

For instance, the net charge of the counter circulating oppositely charged particle is zero, but they constituent a current. Thus, individual charged particles could have charges added to zero.

02

Due to the spin.

The combinations of the different spins forming their total spin do not add to zero. Due to this spin, charged particles constitute magnetic dipole moments.

Conclusion: Yes, an electrically neutral particle composed of charged constituents has a magnetic dipole moment.

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Most popular questions from this chapter

To determine the value of Z at which the relativistic effects might affect energies and whether it applies to all orbiting electrons or to some more than others, also guess if it is acceptable to combine quantum mechanical results.

Whether adding spins to get total spin, spin and orbit to get total angular momentum, or total angular momenta to get a "grand total" angular momentum, addition rules are always the same: Given J1=j1(j1+1)andJ2=j2(j2+1) . Where is an angular momentum (orbital. spin. or total) and a quantum number. the total isJT=jT(jT+1) , where jTmay take on any value between |j1-j2|and j1+j2in integral steps: and for each value ofJJTz=mf . where mmay take on any of2jr+I possible values in integral steps from-jT for +jTSince separately there would be 2j1+1possible values form11 and2j2+ I form2 . the total number of stales should be(2j1+1)(2j2+1) . Prove it: that is, show that the sum of the2jT+1 values formit over all the allowed values forj7 is (2j1+1)(2j2+1). (Note: Here we prove in general what we verified in Example 8.5for the specialcase j1=3,j2=12.)

Slater Determinant: A convenient and compact way of expressing multi-particle states of anti-symmetric character for many fermions is the Slater determinant:

|n1x1m31n2x1m32n3x1m33nNx1msNn1x2m11n2x2m32n3x2m33n1x2msNn3x3m31n2x3m12n3x3m33nNx3msNn1xNm11n2xNm32n3xNm33nNxNmsN|

It is based on the fact that for N fermions there must be Ndifferent individual-particle states, or sets of quantum numbers. The ith state has spatial quantum numbers (which might be ni,i, and mfi) represented simply byni and spin quantum number msi. Were it occupied by the ith particle, the slate would beni(xj)msi a column corresponds to a given state and a row to a given particle. For instance, the first column corresponds to individual particle state n(xj)ms1. Where jprogresses (through the rows) from particle 1 to particle N. The first row corresponds to particle I. which successively occupies all individual-particle states (progressing through the columns). (a) What property of determinants ensures that the multiparticle state is 0 if any two individual particle states are identical? (b) What property of determinants ensures that switching the labels on any two particles switches the sign of the multiparticle state?

The general rule for adding angular momenta is given in Exercise 66, when adding angular momenta withj1=2 and j2=32

(a) What are the possible values of the quantum numberjT and the total angular momentum jT.

(b) How many different states are possible and,

(c) What are the (jT,mjT)values for each of these states?

Question: Discuss what is right or wrong about the following statement:

Nobel gases correspond to full shells.

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