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Table 3 Weights calculated using neighborhood function for triangular lattice

From: CellExcite: an efficient simulation environment for excitable cells

#

0

1

2

3

4

5

6

7

8

d

0

r

3 r MathType@MTEF@5@5@+=feaagaart1ev2aqatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXafv3ySLgzGmvETj2BSbqeeuuDJXwAKbsr4rNCHbGeaGqipu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaaeaabaWaaaGcbiqaaaobdaGcaaqaaKqzWfGaeG4mamdaleqaaOGaemOCaihaaa@344B@

2r

7 r MathType@MTEF@5@5@+=feaagaart1ev2aqatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXafv3ySLgzGmvETj2BSbqeeuuDJXwAKbsr4rNCHbGeaGqipu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaaeaabaWaaaGcbiqaaaobdaGcaaqaaKqzWfGaeG4naCdaleqaaOGaemOCaihaaa@3453@

3r

2 3 r MathType@MTEF@5@5@+=feaagaart1ev2aqatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXafv3ySLgzGmvETj2BSbqeeuuDJXwAKbsr4rNCHbGeaGqipu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaaeaabaWaaaGcbiqaaaobjugCbiabikdaYOWaaOaaaeaajugCbiabiodaZaWcbeaakiabdkhaYbaa@3626@

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

4r

ν r Δ ( d ) MathType@MTEF@5@5@+=feaagaart1ev2aqatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXafv3ySLgzGmvETj2BSbqeeuuDJXwAKbsr4rNCHbGeaGqipu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaaeaabaWaaaGcbaWaaCbiaeaajugCbiabe27aUPWaaSbaaSqaaiabdkhaYbqabaaabeqaaKqzWfGaeyiLdqeaaOWaaeWaaeaacqWGKbazaiaawIcacaGLPaaaaaa@39A1@

−6

1

N/A

N/A

N/A

N/A

N/A

N/A

N/A

ν Δ 2 r ( d ) MathType@MTEF@5@5@+=feaagaart1ev2aqatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXafv3ySLgzGmvETj2BSbqeeuuDJXwAKbsr4rNCHbGeaGqipu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaaeaabaWaaaGcbaWaaCbiaeaajugCbiabe27aUbWcbeqaaKqzWfGaeyiLdqeaaOWaaSbaaSqaaiabikdaYiabdkhaYbqabaGcdaqadaqaaiabdsgaKbGaayjkaiaawMcaaaaa@3A9E@

−42.96

4.48

1.68

1

N/A

N/A

N/A

N/A

N/A

ν Δ 3 r ( d ) MathType@MTEF@5@5@+=feaagaart1ev2aqatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXafv3ySLgzGmvETj2BSbqeeuuDJXwAKbsr4rNCHbGeaGqipu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaaeaabaWaaaGcbaqcfa4aaCbiaOqaaKqzafGaeqyVd4galeqabaqcLbuacqGHuoaraaqcfa4aaSbaaeaacqaIZaWmcqWGYbGCaeqaaiaaykW7daqadaqaaiabdsgaKbGaayjkaiaawMcaaaaa@3CD2@

−191.70

14.39

7.38

5.29

1.94

1

N/A

N/A

N/A

ν Δ 2 r ( d ) MathType@MTEF@5@5@+=feaagaart1ev2aqatCvAUfKttLearuWrP9MDH5MBPbIqV92AaeXafv3ySLgzGmvETj2BSbqeeuuDJXwAKbsr4rNCHbGeaGqipu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq=Jc9vqaqpepm0xbba9pwe9Q8fs0=yqaqpepae9pg0FirpepeKkFr0xfr=xfr=xb9adbaqaaeGaciGaaiaabeqaaeaabaWaaaGcbaWaaCbiaeaajugCbiabe27aUbWcbeqaaKqzWfGaeyiLdqeaaOWaaSbaaSqaaiabikdaYiabdkhaYbqabaGcdaqadaqaaiabdsgaKbGaayjkaiaawMcaaaaa@3A9E@

−726.24

42.52

25.79

20.08

9.48

5.75

2.72

2.12

1