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- NIST/ITL StRD
- Dataset Name: Thurber (Thurber.dat)
- File Format: ASCII
- Starting Values (lines 41 to 47)
- Certified Values (lines 41 to 52)
- Data (lines 61 to 97)
- Procedure: Nonlinear Least Squares Regression
- Description: These data are the result of a NIST study involving
- semiconductor electron mobility. The response
- variable is a measure of electron mobility, and the
- predictor variable is the natural log of the density.
- Reference: Thurber, R., NIST (197?).
- Semiconductor electron mobility modeling.
- Data: 1 Response Variable (y = electron mobility)
- 1 Predictor Variable (x = log[density])
- 37 Observations
- Higher Level of Difficulty
- Observed Data
- Model: Rational Class (cubic/cubic)
- 7 Parameters (b1 to b7)
- y = (b1 + b2*x + b3*x**2 + b4*x**3) /
- (1 + b5*x + b6*x**2 + b7*x**3) + e
- Starting Values Certified Values
- Start 1 Start 2 Parameter Standard Deviation
- b1 = 1000 1300 1.2881396800E+03 4.6647963344E+00
- b2 = 1000 1500 1.4910792535E+03 3.9571156086E+01
- b3 = 400 500 5.8323836877E+02 2.8698696102E+01
- b4 = 40 75 7.5416644291E+01 5.5675370270E+00
- b5 = 0.7 1 9.6629502864E-01 3.1333340687E-02
- b6 = 0.3 0.4 3.9797285797E-01 1.4984928198E-02
- b7 = 0.03 0.05 4.9727297349E-02 6.5842344623E-03
- Residual Sum of Squares: 5.6427082397E+03
- Residual Standard Deviation: 1.3714600784E+01
- Degrees of Freedom: 30
- Number of Observations: 37
- Data: y x
- 80.574E0 -3.067E0
- 84.248E0 -2.981E0
- 87.264E0 -2.921E0
- 87.195E0 -2.912E0
- 89.076E0 -2.840E0
- 89.608E0 -2.797E0
- 89.868E0 -2.702E0
- 90.101E0 -2.699E0
- 92.405E0 -2.633E0
- 95.854E0 -2.481E0
- 100.696E0 -2.363E0
- 101.060E0 -2.322E0
- 401.672E0 -1.501E0
- 390.724E0 -1.460E0
- 567.534E0 -1.274E0
- 635.316E0 -1.212E0
- 733.054E0 -1.100E0
- 759.087E0 -1.046E0
- 894.206E0 -0.915E0
- 990.785E0 -0.714E0
- 1090.109E0 -0.566E0
- 1080.914E0 -0.545E0
- 1122.643E0 -0.400E0
- 1178.351E0 -0.309E0
- 1260.531E0 -0.109E0
- 1273.514E0 -0.103E0
- 1288.339E0 0.010E0
- 1327.543E0 0.119E0
- 1353.863E0 0.377E0
- 1414.509E0 0.790E0
- 1425.208E0 0.963E0
- 1421.384E0 1.006E0
- 1442.962E0 1.115E0
- 1464.350E0 1.572E0
- 1468.705E0 1.841E0
- 1447.894E0 2.047E0
- 1457.628E0 2.200E0
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