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Table 4 Weights calculated using neighborhood function for square lattice

From: CellExcite: an efficient simulation environment for excitable cells

#

0

1

2

3

4

5

6

7

8

9

d

0

r

2 r MathType@MTEF@5@5@+=feaagaart1ev2aqatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXafv3ySLgzGmvETj2BSbqeeuuDJXwAKbsr4rNCHbGeaGqipu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaaeaabaWaaaGcbiqaaaobdaGcaaqaaKqzWfGaeGOmaidaleqaaOGaemOCaihaaa@3449@

2r

5 r MathType@MTEF@5@5@+=feaagaart1ev2aqatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXafv3ySLgzGmvETj2BSbqeeuuDJXwAKbsr4rNCHbGeaGqipu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaaeaabaWaaaGcbiqaaaobdaGcaaqaaKqzWfGaeGynaudaleqaaOGaemOCaihaaa@344F@

2 2 r MathType@MTEF@5@5@+=feaagaart1ev2aqatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXafv3ySLgzGmvETj2BSbqeeuuDJXwAKbsr4rNCHbGeaGqipu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaaeaabaWaaaGcbiqaaaobjugCbiabikdaYOWaaOaaaeaajugCbiabikdaYaWcbeaakiabdkhaYbaa@3624@

3r

10 r MathType@MTEF@5@5@+=feaagaart1ev2aqatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXafv3ySLgzGmvETj2BSbqeeuuDJXwAKbsr4rNCHbGeaGqipu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaaeaabaWaaaGcbiqaaaobdaGcaaqaaKqzWfGaeGymaeJaeGimaadaleqaaOGaemOCaihaaa@3535@

13 r MathType@MTEF@5@5@+=feaagaart1ev2aqatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXafv3ySLgzGmvETj2BSbqeeuuDJXwAKbsr4rNCHbGeaGqipu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaaeaabaWaaaGcbiqaaaobdaGcaaqaaKqzWfGaeGymaeJaeG4mamdaleqaaOGaemOCaihaaa@353B@

4r

ν r ( d ) MathType@MTEF@5@5@+=feaagaart1ev2aqatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXafv3ySLgzGmvETj2BSbqeeuuDJXwAKbsr4rNCHbGeaGqipu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaaeaabaWaaaGcbaWaaCbiaeaajugCbiabe27aUbWcbeqaaKqzWfGaeSyOLCfaaOWaaSbaaSqaaiabdkhaYbqabaGcdaqadaqaaKqzWfGaemizaqgakiaawIcacaGLPaaaaaa@3ADC@

−4

1

N/A

N/A

N/A

N/A

N/A

N/A

N/A

N/A

ν 2 r ( d ) MathType@MTEF@5@5@+=feaagaart1ev2aqatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXafv3ySLgzGmvETj2BSbqeeuuDJXwAKbsr4rNCHbGeaGqipu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaaeaabaWaaaGcbaWaaCbiaeaajugCbiabe27aUbWcbeqaaKqzWfGaeSyOLCfaaOWaaSbaaSqaaiabikdaYiabdkhaYbqabaGcdaqadaqaaKqzWfGaemizaqgakiaawIcacaGLPaaaaaa@3BCE@

−32.8

4:48

2.72

1

N/A

N/A

N/A

N/A

N/A

N/A

ν 3 r ( d ) MathType@MTEF@5@5@+=feaagaart1ev2aqatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXafv3ySLgzGmvETj2BSbqeeuuDJXwAKbsr4rNCHbGeaGqipu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaaeaabaWaaaGcbaWaaCbiaeaajugCbiabe27aUbWcbeqaaKqzWfGaeSyOLCfaaOWaaSbaaSqaaiabiodaZiabdkhaYbqabaGcdaqadaqaaKqzWfGaemizaqgakiaawIcacaGLPaaaaaa@3BD0@

−159.88

14:39

10.31

5.29

3.79

1.40

1

N/A

N/A

N/A

ν 4 r ( d ) MathType@MTEF@5@5@+=feaagaart1ev2aqatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXafv3ySLgzGmvETj2BSbqeeuuDJXwAKbsr4rNCHbGeaGqipu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaaeaabaWaaaGcbaWaaCbiaeaajugCbiabe27aUbWcbeqaaKqzWfGaeSyOLCfaaOWaaSbaaSqaaiabisda0iabdkhaYbqabaGcdaqadaqaaKqzWfGaemizaqgakiaawIcacaGLPaaaaaa@3BD2@

−636.52

42:52

33.12

20.08

15.64

12.18

5.75

4.48

2.12

1