Table 4.

Electron temperatures and densities of IC 2501, Hen 2-7, and PB 4 compared with other works.

ObjectTemperature (K) from CELsTemperature (K) from ORLs
[O iii][Ar iii][N ii][S ii][O ii][O i]He iO iiH i Paschen jump
IC 2501 (This work)9350|$^{+390}_{-390}$|9250|$^{+250}_{-250}$|11 200|$^{+300}_{-300}$|12 600|$^{+4500}_{-2600}$|11 100|$^{+3340}_{-2340}$|9140|$^{+570}_{-450}$|9275|$^{+2212}_{-2275}$|5748|$^{+1431}_{-1282}$|10622
IC 2501 (Model)11 26011 27011 11010 44011 2309742
Milingo et al. (2002b)950011 20011 70010 600
Sharpee et al. (2007)9500|$^{+300}_{-200}$|9400|$^{+600}_{-500}$|10 800|$^{+900}_{-1100}$|12 00013 0006900|$^{+300}_{-200}$|
Hen 2-7 (This work)13 100|$^{+300}_{-300}$|10 700|$^{+400}_{-400}$|11 600|$^{+200}_{-200}$|13 409|$^{+670}_{-670}$|9918|$^{+1190}_{-1190}$|6950|$^{+500}_{-500}$|7017
Hen 2-7 (Model)12 60412 40812 06811 80312 6769885
Cuisinier et al. (1996)11 70011 800
PB 4a (This work)10 000|$^{+500}_{-500}$|14 600|$^{+3000}_{-2800}$|>19 000b3221|$^{+579}_{-965}$|7637
9500|$^{+1000}_{-1000}{}^d$|17800|$^{+2000}_{-2000}{}^d$|
PB 4 (Model)11 05011 02011 02211 01011 01611 009
Cuisinier et al. (1996)9400
ObjectDensity (cm−3) from CELsDensity (cm−3) from ORLs
[O ii][S ii][Cl iii][Ar iv]O iiN iiH i Paschen decrement
IC 2501 (This work)7580|$^{+2590}_{-1690}$|8830|$^{+2140}_{-1600}$|8380|$^{+480}_{-450}$|10700|$^{+2800}_{-2200}$|3980c1270c7874
IC 2501 (Model)8563840185538486
Milingo et al. (2002b)4800
Sharpee et al. (2007)11 000|$^{+9000}_{-4000}$|11 0008500|$^{+2100}_{-1600}$|8775|$^{+2150}_{-1600}$|
Hen 2-7 (This work)1160|$^{+160}_{-140}$|881|$^{+66}_{-61}$|1010|$^{+130}_{-110}$|1600|$^{+370}_{-360}$|1584c7997b
Hen 2-7 (Model)808712807774
Cuisinier et al. (1996)1500
PB 4a (This work)3091|$^{+1220}_{-676}$|2632|$^{+220}_{-200}$|1230:|$^{+710}_{-620}$||$1916^{+1510}_{-1230}$|7080c2300c1061
PB 4 (Model)216918532126
Cuisinier et al. (1996)3970
ObjectTemperature (K) from CELsTemperature (K) from ORLs
[O iii][Ar iii][N ii][S ii][O ii][O i]He iO iiH i Paschen jump
IC 2501 (This work)9350|$^{+390}_{-390}$|9250|$^{+250}_{-250}$|11 200|$^{+300}_{-300}$|12 600|$^{+4500}_{-2600}$|11 100|$^{+3340}_{-2340}$|9140|$^{+570}_{-450}$|9275|$^{+2212}_{-2275}$|5748|$^{+1431}_{-1282}$|10622
IC 2501 (Model)11 26011 27011 11010 44011 2309742
Milingo et al. (2002b)950011 20011 70010 600
Sharpee et al. (2007)9500|$^{+300}_{-200}$|9400|$^{+600}_{-500}$|10 800|$^{+900}_{-1100}$|12 00013 0006900|$^{+300}_{-200}$|
Hen 2-7 (This work)13 100|$^{+300}_{-300}$|10 700|$^{+400}_{-400}$|11 600|$^{+200}_{-200}$|13 409|$^{+670}_{-670}$|9918|$^{+1190}_{-1190}$|6950|$^{+500}_{-500}$|7017
Hen 2-7 (Model)12 60412 40812 06811 80312 6769885
Cuisinier et al. (1996)11 70011 800
PB 4a (This work)10 000|$^{+500}_{-500}$|14 600|$^{+3000}_{-2800}$|>19 000b3221|$^{+579}_{-965}$|7637
9500|$^{+1000}_{-1000}{}^d$|17800|$^{+2000}_{-2000}{}^d$|
PB 4 (Model)11 05011 02011 02211 01011 01611 009
Cuisinier et al. (1996)9400
ObjectDensity (cm−3) from CELsDensity (cm−3) from ORLs
[O ii][S ii][Cl iii][Ar iv]O iiN iiH i Paschen decrement
IC 2501 (This work)7580|$^{+2590}_{-1690}$|8830|$^{+2140}_{-1600}$|8380|$^{+480}_{-450}$|10700|$^{+2800}_{-2200}$|3980c1270c7874
IC 2501 (Model)8563840185538486
Milingo et al. (2002b)4800
Sharpee et al. (2007)11 000|$^{+9000}_{-4000}$|11 0008500|$^{+2100}_{-1600}$|8775|$^{+2150}_{-1600}$|
Hen 2-7 (This work)1160|$^{+160}_{-140}$|881|$^{+66}_{-61}$|1010|$^{+130}_{-110}$|1600|$^{+370}_{-360}$|1584c7997b
Hen 2-7 (Model)808712807774
Cuisinier et al. (1996)1500
PB 4a (This work)3091|$^{+1220}_{-676}$|2632|$^{+220}_{-200}$|1230:|$^{+710}_{-620}$||$1916^{+1510}_{-1230}$|7080c2300c1061
PB 4 (Model)216918532126
Cuisinier et al. (1996)3970

Notes. a PB 4 is defined as optically thin nebula following the criteria proposed by Kaler & Jacoby (1989). The PN spectra shows the absence of [O i] and [N i] lines, weak flux of low-excitation lines such as [O ii] and [N ii], and the very weak flux of [N ii] relative to H α (⁠|$\rm {[N II]/H}\alpha \lt 0.1$|⁠).

b Probably unreliable; c The uncertainty is of order 10–30%; d The value after correction for recombination contribution.

Table 4.

Electron temperatures and densities of IC 2501, Hen 2-7, and PB 4 compared with other works.

ObjectTemperature (K) from CELsTemperature (K) from ORLs
[O iii][Ar iii][N ii][S ii][O ii][O i]He iO iiH i Paschen jump
IC 2501 (This work)9350|$^{+390}_{-390}$|9250|$^{+250}_{-250}$|11 200|$^{+300}_{-300}$|12 600|$^{+4500}_{-2600}$|11 100|$^{+3340}_{-2340}$|9140|$^{+570}_{-450}$|9275|$^{+2212}_{-2275}$|5748|$^{+1431}_{-1282}$|10622
IC 2501 (Model)11 26011 27011 11010 44011 2309742
Milingo et al. (2002b)950011 20011 70010 600
Sharpee et al. (2007)9500|$^{+300}_{-200}$|9400|$^{+600}_{-500}$|10 800|$^{+900}_{-1100}$|12 00013 0006900|$^{+300}_{-200}$|
Hen 2-7 (This work)13 100|$^{+300}_{-300}$|10 700|$^{+400}_{-400}$|11 600|$^{+200}_{-200}$|13 409|$^{+670}_{-670}$|9918|$^{+1190}_{-1190}$|6950|$^{+500}_{-500}$|7017
Hen 2-7 (Model)12 60412 40812 06811 80312 6769885
Cuisinier et al. (1996)11 70011 800
PB 4a (This work)10 000|$^{+500}_{-500}$|14 600|$^{+3000}_{-2800}$|>19 000b3221|$^{+579}_{-965}$|7637
9500|$^{+1000}_{-1000}{}^d$|17800|$^{+2000}_{-2000}{}^d$|
PB 4 (Model)11 05011 02011 02211 01011 01611 009
Cuisinier et al. (1996)9400
ObjectDensity (cm−3) from CELsDensity (cm−3) from ORLs
[O ii][S ii][Cl iii][Ar iv]O iiN iiH i Paschen decrement
IC 2501 (This work)7580|$^{+2590}_{-1690}$|8830|$^{+2140}_{-1600}$|8380|$^{+480}_{-450}$|10700|$^{+2800}_{-2200}$|3980c1270c7874
IC 2501 (Model)8563840185538486
Milingo et al. (2002b)4800
Sharpee et al. (2007)11 000|$^{+9000}_{-4000}$|11 0008500|$^{+2100}_{-1600}$|8775|$^{+2150}_{-1600}$|
Hen 2-7 (This work)1160|$^{+160}_{-140}$|881|$^{+66}_{-61}$|1010|$^{+130}_{-110}$|1600|$^{+370}_{-360}$|1584c7997b
Hen 2-7 (Model)808712807774
Cuisinier et al. (1996)1500
PB 4a (This work)3091|$^{+1220}_{-676}$|2632|$^{+220}_{-200}$|1230:|$^{+710}_{-620}$||$1916^{+1510}_{-1230}$|7080c2300c1061
PB 4 (Model)216918532126
Cuisinier et al. (1996)3970
ObjectTemperature (K) from CELsTemperature (K) from ORLs
[O iii][Ar iii][N ii][S ii][O ii][O i]He iO iiH i Paschen jump
IC 2501 (This work)9350|$^{+390}_{-390}$|9250|$^{+250}_{-250}$|11 200|$^{+300}_{-300}$|12 600|$^{+4500}_{-2600}$|11 100|$^{+3340}_{-2340}$|9140|$^{+570}_{-450}$|9275|$^{+2212}_{-2275}$|5748|$^{+1431}_{-1282}$|10622
IC 2501 (Model)11 26011 27011 11010 44011 2309742
Milingo et al. (2002b)950011 20011 70010 600
Sharpee et al. (2007)9500|$^{+300}_{-200}$|9400|$^{+600}_{-500}$|10 800|$^{+900}_{-1100}$|12 00013 0006900|$^{+300}_{-200}$|
Hen 2-7 (This work)13 100|$^{+300}_{-300}$|10 700|$^{+400}_{-400}$|11 600|$^{+200}_{-200}$|13 409|$^{+670}_{-670}$|9918|$^{+1190}_{-1190}$|6950|$^{+500}_{-500}$|7017
Hen 2-7 (Model)12 60412 40812 06811 80312 6769885
Cuisinier et al. (1996)11 70011 800
PB 4a (This work)10 000|$^{+500}_{-500}$|14 600|$^{+3000}_{-2800}$|>19 000b3221|$^{+579}_{-965}$|7637
9500|$^{+1000}_{-1000}{}^d$|17800|$^{+2000}_{-2000}{}^d$|
PB 4 (Model)11 05011 02011 02211 01011 01611 009
Cuisinier et al. (1996)9400
ObjectDensity (cm−3) from CELsDensity (cm−3) from ORLs
[O ii][S ii][Cl iii][Ar iv]O iiN iiH i Paschen decrement
IC 2501 (This work)7580|$^{+2590}_{-1690}$|8830|$^{+2140}_{-1600}$|8380|$^{+480}_{-450}$|10700|$^{+2800}_{-2200}$|3980c1270c7874
IC 2501 (Model)8563840185538486
Milingo et al. (2002b)4800
Sharpee et al. (2007)11 000|$^{+9000}_{-4000}$|11 0008500|$^{+2100}_{-1600}$|8775|$^{+2150}_{-1600}$|
Hen 2-7 (This work)1160|$^{+160}_{-140}$|881|$^{+66}_{-61}$|1010|$^{+130}_{-110}$|1600|$^{+370}_{-360}$|1584c7997b
Hen 2-7 (Model)808712807774
Cuisinier et al. (1996)1500
PB 4a (This work)3091|$^{+1220}_{-676}$|2632|$^{+220}_{-200}$|1230:|$^{+710}_{-620}$||$1916^{+1510}_{-1230}$|7080c2300c1061
PB 4 (Model)216918532126
Cuisinier et al. (1996)3970

Notes. a PB 4 is defined as optically thin nebula following the criteria proposed by Kaler & Jacoby (1989). The PN spectra shows the absence of [O i] and [N i] lines, weak flux of low-excitation lines such as [O ii] and [N ii], and the very weak flux of [N ii] relative to H α (⁠|$\rm {[N II]/H}\alpha \lt 0.1$|⁠).

b Probably unreliable; c The uncertainty is of order 10–30%; d The value after correction for recombination contribution.

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