Table 2

Power series fitted to energy transfer rates

State

(010)

-37.98

3.32

-1.76 × 10^-1

5.37 × 10^-3

-1.02 × 10^-4

(100)+(001)

-53.94

4.72

-2.28 × 10^-1

6.44 × 10^-3

-1.14 × 10^-4

B₁

-192.48

7.40

-2.72 × 10^-2

-4.93 × 10^-3

1.50 × 10^-4

B₁

-182.22

5.46

9.05 × 10^-2

-8.62 × 10^-3

2.18 × 10^-4

³A₂

-217.11

6.49

1.05 × 10^-1

-9.87 × 10^-3

2.46 × 10^-4

¹A₂

-175.83

3.05

2.18 × 10^-1

-1.17 × 10^-2

2.57 × 10^-4

A₁

-187.82

3.90

1.88 × 10^-1

-1.10 × 10^-2

2.47 × 10^-4

A₁

-205.30

4.71

1.88 × 10^-1

-1.19 × 10^-2

2.73 × 10^-4

A₁

-185.00

1.59

3.65 × 10^-1

-1.72 × 10^-2

3.68 × 10^-4

B₁+B₁

-198.45

1.04

4.71 × 10^-1

-2.18 × 10^-2

4.71 × 10^-4

A₁

-190.37

1.68

3.75 × 10^-1

-1.77 × 10^-2

3.79 × 10^-4

B₁(100)+³B₁

-252.84

6.34

2.37 × 10^-1

-1.58 × 10^-2

3.74 × 10^-4

¹B₁+A₁(100)

-235.91

6.31

1.56 × 10^-1

-1.17 × 10^-2

2.76 × 10^-4

³A₂

-255.52

6.76

1.97 × 10^-1

-1.41 × 10^-2

3.35 × 10^-4

A₁(110)+B₁(200)

-232.55

6.21

1.36 × 10^-1

-1.04 × 10^-2

2.43 × 10^-4

¹A₂

-218.73

3.60

3.04 × 10^-1

-1.58 × 10^-2

3.46 × 10^-4

B₁+B₁+A₁(200)

-214.99

3.31

3.12 × 10^-1

-1.60 × 10^-2

3.47 × 10^-4

³B₂+¹B₂+³B₂

-253.22

4.24

3.92 × 10^-1

-2.08 × 10^-2

4.64 × 10^-4

³A₁+¹A₂+¹A₁+³A₂+¹B₁+³B₁

-340.25

12.15

7.66 × 10^-2

-1.36 × 10^-2

3.62 × 10^-4

¹B₁+³B₁+³A₁+¹A₁

-320.73

11.00

9.06 × 10^-2

-1.31 × 10^-2

3.40 × 10^-4

¹B₂+³B₂+³B₁+¹B₁

-250.50

5.83

2.29 × 10^-1

-1.43 × 10^-2

3.25 × 10^-4

³A₂+¹A₂

-211.30

2.77

3.18 × 10^-1

-1.54 × 10^-2

3.24 × 10^-4

³B₁

-255.49

3.63

4.29 × 10^-1

-2.16 × 10^-2

4.71 × 10^-4

¹B₁

-206.46

2.94

2.80 × 10^-1

-1.37 × 10^-2

2.86 × 10^-4

³A₁+¹A₁

-218.13

3.36

2.91 × 10^-1

-1.46 × 10^-2

3.10 × 10^-4

¹A₁+³B₁+¹B₁

-244.26

4.12

3.34 × 10^-1

-1.75 × 10^-2

3.80 × 10^-4

¹A₁

-217.71

3.18

3.01 × 10^-1

-1.49 × 10-2

3.14 × 10^-4

State

(010)

1.23 × 10^-6

-9.06 × 10^-9

3.75 × 10^-11

6.66 × 10^-14

(100)+(001)

1.29 × 10^-6

-9.02 × 10^-9

3.56 × 10^-11

-6.06 × 10^-14

B₁

-2.12 × 10^-6

1.67 × 10^-8

-6.99 × 10^-11

1.23 × 10^-13

B₁

-2.91 × 10^-6

2.22 × 10^-8

-9.16 × 10^-11

1.59 × 10^-13

³A₂

-3.23 × 10^-6

2.42 × 10^-8

-9.82 × 10^-11

1.68 × 10^-13

¹A₂

-3.17 × 10^-6

2.28 × 10^-8

-8.96 × 10^-11

1.50 × 10^-13

A₁

-3.06 × 10^-6

2.20 × 10^-8

-8.66 × 10^-11

1.44 × 10^-13

A₁

-3.45 × 10^-6

2.52 × 10^-8

-1.00 × 10^-10

1.69 × 10^-13

A₁

-4.49 × 10^-6

3.21 × 10^-8

-1.26 × 10^-10

2.10 × 10^-13

B₁+B₁

-5.80 × 10^-6

4.19 × 10^-8

-1.66 × 10^-10

2.79 × 10^-13

A₁

-4.63 × 10^-6

3.31 × 10^-8

-1.30 × 10^-10

2.17 × 10^-13

B₁(100)+³B₁

-4.80 × 10^-6

3.55 × 10^-8

-1.43 × 10^-10

2.43 × 10^-13

¹B₁+A₁(100)

-3.50 × 10^-6

2.55 × 10^-8

-1.01 × 10^-10

1.69 × 10^-13

³A₂

-4.28 × 10^-6

3.15 × 10^-8

-1.26 × 10^-10

2.12 × 10^-13

A₁(110)+B₁(200)

-3.04 × 10^-6

2.18 × 10^-8

-8.50 × 10^-11

1.40 × 10^-13

¹A₂

-4.23 × 10^-6

3.01 × 10^-8

-1.17 × 10^-10

1.93 × 10^-13

B₁+B₁+A₁(200)

-4.24 × 10^-6

3.02 × 10^-8

-1.18 × 10^-10

1.94 × 10^-13

³B₂+¹B₂+³B₂

-5.76 × 10^-6

4.16 × 10^-8

-1.64 × 10^-10

2.74 × 10^-13

³A₁+¹A₂+¹A₁+³A₂+¹B₁+³B₁

-4.85 × 10^-6

3.65 × 10^-8

-1.48 × 10^-10

2.52 × 10^-13

¹B₁+³B₁+³A₁+¹A₁

-4.51 × 10^-6

3.38 × 10^-8

-1.36 × 10^-10

2.31 × 10^-13

¹B₂+³B₂+³B₁+¹B₁

-4.02 × 10^-6

2.88 × 10^-8

-1.12 × 10^-10

1.85 × 10^-13

³A₂+¹A₂

-3.86 × 10^-6

2.68 × 10^-8

-1.02 × 10^-10

1.66 × 10^-13

³B₁

-5.75 × 10^-6

4.09 × 10^-8

-1.59 × 10^-10

2.63 × 10^-13

¹B₁

-3.37 × 10^-6

2.32 × 10^-8

-8.75 × 10^-11

1.40 × 10^-13

³A₁+¹A₁

-3.69 × 10^-6

2.56 × 10^-8

-9.75 × 10^-11

1.57 × 10^-13

¹A₁+³B₁+¹B₁

-4.61 × 10^-6

3.26 × 10^-8

-1.26 × 10^-10

2.06 × 10^-13

¹A₁

-3.72 × 10^-6

2.58 × 10^-8

-9.82 × 10^-11

1.58 × 10^-13

Coefficients that result from the fitting of a power series to our computed electron energy transfer rates. The vibrational and electronic state transitions are labelled in the first column.

Thorn et al. PMC Physics B 2009 2:1   doi:10.1186/1754-0429-2-1