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(a) Construct the spatial wave function ()for hydrogen in the state n=3,I=2,m=1.Express your answer as a function of r,,,anda(the Bohr radius) only鈥攏o other variables (p,z,etc.) or functions (p,v,etc.), or constants (A,c0,etc.), or derivatives, allowed (蟺 is okay, and e, and 2, etc.).

(b) Check that this wave function is properly normalized, by carrying out the appropriate integrals over, ,and.

(c) Find the expectation value of rsin this state. For what range of s (positive and negative) is the result finite?

Short Answer

Expert verified

(a)321=R32Y21=-1181a7/2r2e-r/3a蝉颈苍胃肠辞蝉胃别颈蠒.

(b)The wave function is properly normalized by 1

(C)rs=-7.

Step by step solution

01

(a) Constructing the spatial wave function for hydrogen.

321=R32Y21=481301a3/2ra2e-r/3a-158蝉颈苍胃肠辞蝉胃别颈蠒=-1181a7/2r2e-r/3a蝉颈苍胃肠辞蝉胃别颈蠒.

02

 Step2: (b) Checking the wave function is properly normalized.

2d3r=11812a7r4e-2r/3asin2cos2r2sindrdd.=1812a720r6e-2r/3adr01-cos2cos2cos2d.=2812a76!3a27-cos33+cos550.=238a76.5.4.3.237a72723-25=3.54.415=1.

03

 Step3: (c)Finding the exceptional value of rs

rs=0rsR322r2dr=48121301a70rs+6e-2r/3adr.=815812a7s+6!3a2s+7=s+6!3a251720=(s+6)!6!3a23.FiniteforS>-7.

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Most popular questions from this chapter

(a) Work out the Clebsch-Gordan coefficients for the case s1=1/2,s2=anything. Hint: You're looking for the coefficients A and Bin

|sm=A|1212|s2(m-12)+B|12(-12)|s2(m+12)

such that|sm is an eigenstate of . Use the method of Equations 4.179 through 4.182. If you can't figure out whatSx(2) (for instance) does to|s2m2 , refer back to Equation 4.136 and the line before Equation 4.147. Answer:

;role="math" localid="1658209512756" A=s2+12m2s2+1;B=s2+12m2s2+1

where, the signs are determined bys=s21/2 .

(b) Check this general result against three or four entries in Table 4.8.

Work out the spin matrices for arbitrary spin , generalizing spin (Equations 4.145 and 4.147), spin 1 (Problem 4.31), and spin (Problem 4.52). Answer:

Sz=(s0000s-10000s-200000-s)Sx=2(0bs0000bs0bs-10000bs-10bs-20000bs-200000000b-s+10000b-s+10)Sy=2(0-ibs0000ibs0-ibs-10000-ibs-10-ibs-20000-ibs-200000000-ibs+10000-ibs+10)

where,bj(s+j)(s+1-j)

A hydrogenic atom consists of a single electron orbiting a nucleus with Z protons. (Z=1 would be hydrogen itself,Z=2is ionized helium ,Z=3is doubly ionized lithium, and so on.) Determine the Bohr energies En(Z), the binding energyE1(Z), the Bohr radiusa(Z), and the Rydberg constant R(Z)for a hydrogenic atom. (Express your answers as appropriate multiples of the hydrogen values.) Where in the electromagnetic spectrum would the Lyman series fall, for Z=2and Z=3? Hint: There鈥檚 nothing much to calculate here鈥 in the potential (Equation 4.52) Ze2, so all you have to do is make the same substitution in all the final results.

V(r)=-e24o01r (4.52).

(a) Find鈱﹔鈱猘nd鈱﹔虏鈱猣or an electron in the ground state of hydrogen. Express your answers in terms of the Bohr radius.

(b) Find鈱﹛鈱猘nd (x2)for an electron in the ground state of hydrogen.

Hint: This requires no new integration鈥攏ote that r2=x2+y2+z2,and exploit the symmetry of the ground state.

(c) Find鈱﹛虏鈱猧n the state n=2,l=1,m=1. Hint: this state is not symmetrical in x, y, z. Usex=rsincosx=rsincos

Use Equation 4.32 to construct Yll(,)andy32(.) . (You can take P32from Table 4.2, but you'll have to work outPll from Equations 4.27 and 4.28.) Check that they satisfy the angular equation (Equation 4.18), for the appropriate values of l and m .

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