LİSANS FİZİĞİ

  (10)     n = 3  ~   l = 2    ~  m = 2

    Ψ322 (r,θ,φ) = R32 (r) Y2² (θ,φ)

       Y2² (θ,φ) = [15/32π]¹/² (sin²θ) exp(2iφ)

    Ψ322 =(2/27)[3/16π]¹/² (z/3a)³/² (zr/a)² (sin²θ) exp[-(zr/3a)+2iφ]

   (11)     n = 3  ~   l = 1    ~  m = -1

                                                  -1

    Ψ31-1 (r,θ,φ) = R31 (r) Y1 (θ,φ)

        R31(r) = (4/9)(2)¹/² (z/3a)³/²(zr/a) (1 -[zr/6a]) exp(-zr/3a)

          -1

        Y1 (θ,φ) = [3/8π]¹/² (sinθ) exp(-iφ)

    Ψ31-1 =  (4/9)[3/4π]¹/² (z/3a)³/²(zr/a)(sinθ) (1 -[zr/6a]) exp(-(zr/3a)-iφ)

   (12)     n = 3  ~   l = 1    ~  m = 0

    Ψ310 (r,θ,φ) = R31 (r) Y1º (θ,φ) 

        Y1º (θ,φ) = [3/4π]¹/² (cosθ)

    Ψ310 = (4/9)[3/2π]¹/² (z/3a)³/²(zr/a)(cosθ)(1 -[zr/6a]) exp(-zr/3a)

   (13)     n = 3  ~   l = 1    ~  m = 1

    Ψ311 (r,θ,φ) = R31 (r) Y1¹ (θ,φ) 

        Y1¹ (θ,φ) = -  [3/8π]¹/² (sinθ) exp(iφ)

    Ψ311 =-(4/9)[3/4π]¹/²(z/3a)³/²(zr/a)(sinθ)(1 -[zr/6a]) exp(-(zr/3a)+iφ)

   (14)     n = 3  ~   l = 0    ~  m = 0

    Ψ300 (r,θ,φ) = R30 (r) Y0º (θ,φ)  

        R30(r) = 2 (z/3a)³/² [1- (2zr/3a)+(2z²r²/27a²)] exp (-zr/3a)

        Y0º (θ,φ) = [1/4π]¹/²

    Ψ300  =  2 [1/4π]¹/²(z/3a)³/² [1- (2zr/3a)+(2z²r²/27a²)] exp (-zr/3a)

                                     GERİ  DÖN