Table 3. Open in new tab Photometric...

Parameter

2015

2016(a)

2016(b)

2015

2016(a)

2016(b)

|$T_{1}(K)$|

4100(fixed)

4317(fixed)

|$g_{1}$| = |$g_{2}$|

0.32(fixed)

|$A_{1}$| = |$A_{2}$|

0.50(fixed)

|$x_{1}$| = |$x_{2} (B$|⁠)

0.828

...

0.831

0.830

...

|$x_{1}$| = |$x_{2} (V$|⁠)

0.793

0.792

0.793

0.794

|$x_{1}$| = |$x_{2} (R_{\rm c}$|⁠)

0.760

0.759

|$x_{1}$| = |$x_{2} (I_{\rm c}$|⁠)

0.675

0.676

|$y_{1}$| = |$y_{2} (B$|⁠)

0.089

0.087

...

|$-$|0.080

...

|$y_{1}$| = |$y_{2} (V$|⁠)

0.188

0.187

0.184

0.080

|$y_{1}$| = |$y_{2} (R_{\rm c}$|⁠)

0.232

0.231

0.160

|$y_{1}$| = |$y_{2} (I_{\rm c}$|⁠)

0.262

0.261

0.220

q (⁠|$M_2/M_1$|⁠)

1.26(7)

1.15(2)

1.08(4)

1.26(6)

1.06(1)

1.10(1)

|$i\ (^{\circ })$|

78.0(fixed)

77.9(4)

78.2(2)

78.0(fixed)

77.8(4)

78.1(3)

|$\Omega _{\rm in}$|

4.1601

3.9969

3.8681

4.1601

3.8250

3.9108

|$\Omega _{\rm out}$|

3.5965

3.4406

3.3185

3.5965

3.2777

3.3588

|$\Omega _{1}=\Omega _{2}$|

4.0399(59)

4.0782(66)

3.7611(575)

4.0383(131)

3.7455(218)

3.8196(116)

|$T_{2}\ (K)$|

3895(5)

3894(15)

3917(17)

4104(6)

4111(3)

4126(3)

|$L_{1}/(L_{1}+L_{2}+L_{3}$|⁠) (B)

55.14|$\%$|

56.68|$\%$|

...

54.50|$\%$|

58.05|$\%$|

...

|$L_{1}/(L_{1}+L_{2}+L_{3}$|⁠) (V)

53.30|$\%$|

55.00|$\%$|

55.72|$\%$|

52.70|$\%$|

56.54|$\%$|

54.98|$\%$|

|$L_{1}/(L_{1}+L_{2}+L_{3}$|⁠) (R)

51.93|$\%$|

53.39|$\%$|

54.24|$\%$|

51.41|$\%$|

54.91|$\%$|

53.48|$\%$|

|$L_{1}/(L_{1}+L_{2}+L_{3}$|⁠) (I)

49.75|$\%$|

50.82|$\%$|

51.76|$\%$|

49.40|$\%$|

52.45|$\%$|

50.73|$\%$|

|$L_{3}/(L_{1}+L_{2}+L_{3}$|⁠) (B)

1.4(0.6)|$\%$|

1.8(1.5)|$\%$|

2.5(1.5)|$\%$|

2.9(0.5)|$\%$|

...

|$L_{3}/(L_{1}+L_{2}+L_{3}$|⁠) (V)

1.9(0.7)|$\%$|

1.8(1.5)|$\%$|

2.6(1.9)|$\%$|

2.7(0.6)|$\%$|

2.0(1.1)|$\%$|

2.3(0.5)|$\%$|

|$L_{3}/(L_{1}+L_{2}+L_{3}$|⁠) (R)

2.6(0.6)|$\%$|

3.1(1.4)|$\%$|

3.9(1.9)|$\%$|

3.2(0.5)|$\%$|

2.5(1.2)|$\%$|

2.8(0.3)|$\%$|

|$L_{3}/(L_{1}+L_{2}+L_{3}$|⁠) (I)

3.4(0.6)|$\%$|

4.6(1.4)|$\%$|

5.6(1.8)|$\%$|

4.8(0.3)|$\%$|

4.1(1.1)|$\%$|

4.2(0.5)|$\%$|

|$r_{1}$| (pole)

0.3509(7)

0.3569(19)

0.3636(32)

0.3510(15)

0.3637(14)

0.3591(10)

|$r_{1}$| (side)

0.3700(9)

0.3765(21)

0.3841(36)

0.3702(19)

0.3839(17)

0.3786(11)

|$r_{1}$| (back)

0.4101(14)

0.4153(24)

0.4329(38)

0.4103(29)

0.4220(21)

0.4154(11)

|$r_{2}$| (pole)

0.3891(7)

0.3825(64)

0.3747(111)

0.3893(15)

0.3736(41)

0.3725(35)

|$r_{2}$| (side)

0.4127(8)

0.4052(82)

0.3962(142)

0.4129(19)

0.3950(53)

0.3934(44)

|$r_{2}$| (back)

0.4497(13)

0.4431(13)

0.4335(227)

0.4490(28)

0.4325(83)

0.4287(69)

21.1(1.4)|$\%$|

21.0(6.3)|$\%$|

19.5(10.5)|$\%$|

21.6(2.3)|$\%$|

18.7(3.9)|$\%$|

16.5(2.1)|$\%$|

|$\Sigma$| res|$^{2}$|

0.0298

0.0116

0.0122

0.0104

0.0010

0.0111

Parameter

2015

2016(a)

2016(b)

2015

2016(a)

2016(b)

|$T_{1}(K)$|

4100(fixed)

4317(fixed)

|$g_{1}$| = |$g_{2}$|

0.32(fixed)

|$A_{1}$| = |$A_{2}$|

0.50(fixed)

|$x_{1}$| = |$x_{2} (B$|⁠)

0.828

...

0.831

0.830

...

|$x_{1}$| = |$x_{2} (V$|⁠)

0.793

0.792

0.793

0.794

|$x_{1}$| = |$x_{2} (R_{\rm c}$|⁠)

0.760

0.759

|$x_{1}$| = |$x_{2} (I_{\rm c}$|⁠)

0.675

0.676

|$y_{1}$| = |$y_{2} (B$|⁠)

0.089

0.087

...

|$-$|0.080

...

|$y_{1}$| = |$y_{2} (V$|⁠)

0.188

0.187

0.184

0.080

|$y_{1}$| = |$y_{2} (R_{\rm c}$|⁠)

0.232

0.231

0.160

|$y_{1}$| = |$y_{2} (I_{\rm c}$|⁠)

0.262

0.261

0.220

q (⁠|$M_2/M_1$|⁠)

1.26(7)

1.15(2)

1.08(4)

1.26(6)

1.06(1)

1.10(1)

|$i\ (^{\circ })$|

78.0(fixed)

77.9(4)

78.2(2)

78.0(fixed)

77.8(4)

78.1(3)

|$\Omega _{\rm in}$|

4.1601

3.9969

3.8681

4.1601

3.8250

3.9108

|$\Omega _{\rm out}$|

3.5965

3.4406

3.3185

3.5965

3.2777

3.3588

|$\Omega _{1}=\Omega _{2}$|

4.0399(59)

4.0782(66)

3.7611(575)

4.0383(131)

3.7455(218)

3.8196(116)

|$T_{2}\ (K)$|

3895(5)

3894(15)

3917(17)

4104(6)

4111(3)

4126(3)

|$L_{1}/(L_{1}+L_{2}+L_{3}$|⁠) (B)

55.14|$\%$|

56.68|$\%$|

...

54.50|$\%$|

58.05|$\%$|

...

|$L_{1}/(L_{1}+L_{2}+L_{3}$|⁠) (V)

53.30|$\%$|

55.00|$\%$|

55.72|$\%$|

52.70|$\%$|

56.54|$\%$|

54.98|$\%$|

|$L_{1}/(L_{1}+L_{2}+L_{3}$|⁠) (R)

51.93|$\%$|

53.39|$\%$|

54.24|$\%$|

51.41|$\%$|

54.91|$\%$|

53.48|$\%$|

|$L_{1}/(L_{1}+L_{2}+L_{3}$|⁠) (I)

49.75|$\%$|

50.82|$\%$|

51.76|$\%$|

49.40|$\%$|

52.45|$\%$|

50.73|$\%$|

|$L_{3}/(L_{1}+L_{2}+L_{3}$|⁠) (B)

1.4(0.6)|$\%$|

1.8(1.5)|$\%$|

2.5(1.5)|$\%$|

2.9(0.5)|$\%$|

...

|$L_{3}/(L_{1}+L_{2}+L_{3}$|⁠) (V)

1.9(0.7)|$\%$|

1.8(1.5)|$\%$|

2.6(1.9)|$\%$|

2.7(0.6)|$\%$|

2.0(1.1)|$\%$|

2.3(0.5)|$\%$|

|$L_{3}/(L_{1}+L_{2}+L_{3}$|⁠) (R)

2.6(0.6)|$\%$|

3.1(1.4)|$\%$|

3.9(1.9)|$\%$|

3.2(0.5)|$\%$|

2.5(1.2)|$\%$|

2.8(0.3)|$\%$|

|$L_{3}/(L_{1}+L_{2}+L_{3}$|⁠) (I)

3.4(0.6)|$\%$|

4.6(1.4)|$\%$|

5.6(1.8)|$\%$|

4.8(0.3)|$\%$|

4.1(1.1)|$\%$|

4.2(0.5)|$\%$|

|$r_{1}$| (pole)

0.3509(7)

0.3569(19)

0.3636(32)

0.3510(15)

0.3637(14)

0.3591(10)

|$r_{1}$| (side)

0.3700(9)

0.3765(21)

0.3841(36)

0.3702(19)

0.3839(17)

0.3786(11)

|$r_{1}$| (back)

0.4101(14)

0.4153(24)

0.4329(38)

0.4103(29)

0.4220(21)

0.4154(11)

|$r_{2}$| (pole)

0.3891(7)

0.3825(64)

0.3747(111)

0.3893(15)

0.3736(41)

0.3725(35)

|$r_{2}$| (side)

0.4127(8)

0.4052(82)

0.3962(142)

0.4129(19)

0.3950(53)

0.3934(44)

|$r_{2}$| (back)

0.4497(13)

0.4431(13)

0.4335(227)

0.4490(28)

0.4325(83)

0.4287(69)

21.1(1.4)|$\%$|

21.0(6.3)|$\%$|

19.5(10.5)|$\%$|

21.6(2.3)|$\%$|

18.7(3.9)|$\%$|

16.5(2.1)|$\%$|

|$\Sigma$| res|$^{2}$|

0.0298

0.0116

0.0122

0.0104

0.0010

0.0111

Table 3.

Open in new tab

Photometric solutions for J161335.

Parameter	2015	2016(a)	2016(b)	2015	2016(a)	2016(b)
\|$T_{1}(K)$\|	4100(fixed)	4100(fixed)	4100(fixed)	4317(fixed)	4317(fixed)	4317(fixed)
\|$g_{1}$\| = \|$g_{2}$\|	0.32(fixed)	0.32(fixed)	0.32(fixed)	0.32(fixed)	0.32(fixed)	0.32(fixed)
\|$A_{1}$\| = \|$A_{2}$\|	0.50(fixed)	0.50(fixed)	0.50(fixed)	0.50(fixed)	0.50(fixed)	0.50(fixed)
\|$x_{1}$\| = \|$x_{2} (B$\|⁠)	0.828	0.828	...	0.831	0.830	...
\|$x_{1}$\| = \|$x_{2} (V$\|⁠)	0.793	0.792	0.792	0.793	0.794	0.794
\|$x_{1}$\| = \|$x_{2} (R_{\rm c}$\|⁠)	0.760	0.760	0.760	0.760	0.759	0.759
\|$x_{1}$\| = \|$x_{2} (I_{\rm c}$\|⁠)	0.675	0.675	0.675	0.676	0.676	0.676
\|$y_{1}$\| = \|$y_{2} (B$\|⁠)	0.089	0.087	...	\|$-$\|0.080	\|$-$\|0.080	...
\|$y_{1}$\| = \|$y_{2} (V$\|⁠)	0.188	0.187	0.184	0.080	0.080	0.080
\|$y_{1}$\| = \|$y_{2} (R_{\rm c}$\|⁠)	0.232	0.232	0.231	0.160	0.160	0.160
\|$y_{1}$\| = \|$y_{2} (I_{\rm c}$\|⁠)	0.262	0.261	0.261	0.220	0.220	0.220
q (⁠\|$M_2/M_1$\|⁠)	1.26(7)	1.15(2)	1.08(4)	1.26(6)	1.06(1)	1.10(1)
\|$i\ (^{\circ })$\|	78.0(fixed)	77.9(4)	78.2(2)	78.0(fixed)	77.8(4)	78.1(3)
\|$\Omega _{\rm in}$\|	4.1601	3.9969	3.8681	4.1601	3.8250	3.9108
\|$\Omega _{\rm out}$\|	3.5965	3.4406	3.3185	3.5965	3.2777	3.3588
\|$\Omega _{1}=\Omega _{2}$\|	4.0399(59)	4.0782(66)	3.7611(575)	4.0383(131)	3.7455(218)	3.8196(116)
\|$T_{2}\ (K)$\|	3895(5)	3894(15)	3917(17)	4104(6)	4111(3)	4126(3)
\|$L_{1}/(L_{1}+L_{2}+L_{3}$\|⁠) (B)	55.14\|$\%$\|	56.68\|$\%$\|	...	54.50\|$\%$\|	58.05\|$\%$\|	...
\|$L_{1}/(L_{1}+L_{2}+L_{3}$\|⁠) (V)	53.30\|$\%$\|	55.00\|$\%$\|	55.72\|$\%$\|	52.70\|$\%$\|	56.54\|$\%$\|	54.98\|$\%$\|
\|$L_{1}/(L_{1}+L_{2}+L_{3}$\|⁠) (R)	51.93\|$\%$\|	53.39\|$\%$\|	54.24\|$\%$\|	51.41\|$\%$\|	54.91\|$\%$\|	53.48\|$\%$\|
\|$L_{1}/(L_{1}+L_{2}+L_{3}$\|⁠) (I)	49.75\|$\%$\|	50.82\|$\%$\|	51.76\|$\%$\|	49.40\|$\%$\|	52.45\|$\%$\|	50.73\|$\%$\|
\|$L_{3}/(L_{1}+L_{2}+L_{3}$\|⁠) (B)	1.4(0.6)\|$\%$\|	1.8(1.5)\|$\%$\|	2.5(1.5)\|$\%$\|	2.9(0.5)\|$\%$\|	...
\|$L_{3}/(L_{1}+L_{2}+L_{3}$\|⁠) (V)	1.9(0.7)\|$\%$\|	1.8(1.5)\|$\%$\|	2.6(1.9)\|$\%$\|	2.7(0.6)\|$\%$\|	2.0(1.1)\|$\%$\|	2.3(0.5)\|$\%$\|
\|$L_{3}/(L_{1}+L_{2}+L_{3}$\|⁠) (R)	2.6(0.6)\|$\%$\|	3.1(1.4)\|$\%$\|	3.9(1.9)\|$\%$\|	3.2(0.5)\|$\%$\|	2.5(1.2)\|$\%$\|	2.8(0.3)\|$\%$\|
\|$L_{3}/(L_{1}+L_{2}+L_{3}$\|⁠) (I)	3.4(0.6)\|$\%$\|	4.6(1.4)\|$\%$\|	5.6(1.8)\|$\%$\|	4.8(0.3)\|$\%$\|	4.1(1.1)\|$\%$\|	4.2(0.5)\|$\%$\|
\|$r_{1}$\| (pole)	0.3509(7)	0.3569(19)	0.3636(32)	0.3510(15)	0.3637(14)	0.3591(10)
\|$r_{1}$\| (side)	0.3700(9)	0.3765(21)	0.3841(36)	0.3702(19)	0.3839(17)	0.3786(11)
\|$r_{1}$\| (back)	0.4101(14)	0.4153(24)	0.4329(38)	0.4103(29)	0.4220(21)	0.4154(11)
\|$r_{2}$\| (pole)	0.3891(7)	0.3825(64)	0.3747(111)	0.3893(15)	0.3736(41)	0.3725(35)
\|$r_{2}$\| (side)	0.4127(8)	0.4052(82)	0.3962(142)	0.4129(19)	0.3950(53)	0.3934(44)
\|$r_{2}$\| (back)	0.4497(13)	0.4431(13)	0.4335(227)	0.4490(28)	0.4325(83)	0.4287(69)
f	21.1(1.4)\|$\%$\|	21.0(6.3)\|$\%$\|	19.5(10.5)\|$\%$\|	21.6(2.3)\|$\%$\|	18.7(3.9)\|$\%$\|	16.5(2.1)\|$\%$\|
\|$\Sigma$\| res\|$^{2}$\|	0.0298	0.0116	0.0122	0.0104	0.0010	0.0111

Parameter	2015	2016(a)	2016(b)	2015	2016(a)	2016(b)
\|$T_{1}(K)$\|	4100(fixed)	4100(fixed)	4100(fixed)	4317(fixed)	4317(fixed)	4317(fixed)
\|$g_{1}$\| = \|$g_{2}$\|	0.32(fixed)	0.32(fixed)	0.32(fixed)	0.32(fixed)	0.32(fixed)	0.32(fixed)
\|$A_{1}$\| = \|$A_{2}$\|	0.50(fixed)	0.50(fixed)	0.50(fixed)	0.50(fixed)	0.50(fixed)	0.50(fixed)
\|$x_{1}$\| = \|$x_{2} (B$\|⁠)	0.828	0.828	...	0.831	0.830	...
\|$x_{1}$\| = \|$x_{2} (V$\|⁠)	0.793	0.792	0.792	0.793	0.794	0.794
\|$x_{1}$\| = \|$x_{2} (R_{\rm c}$\|⁠)	0.760	0.760	0.760	0.760	0.759	0.759
\|$x_{1}$\| = \|$x_{2} (I_{\rm c}$\|⁠)	0.675	0.675	0.675	0.676	0.676	0.676
\|$y_{1}$\| = \|$y_{2} (B$\|⁠)	0.089	0.087	...	\|$-$\|0.080	\|$-$\|0.080	...
\|$y_{1}$\| = \|$y_{2} (V$\|⁠)	0.188	0.187	0.184	0.080	0.080	0.080
\|$y_{1}$\| = \|$y_{2} (R_{\rm c}$\|⁠)	0.232	0.232	0.231	0.160	0.160	0.160
\|$y_{1}$\| = \|$y_{2} (I_{\rm c}$\|⁠)	0.262	0.261	0.261	0.220	0.220	0.220
q (⁠\|$M_2/M_1$\|⁠)	1.26(7)	1.15(2)	1.08(4)	1.26(6)	1.06(1)	1.10(1)
\|$i\ (^{\circ })$\|	78.0(fixed)	77.9(4)	78.2(2)	78.0(fixed)	77.8(4)	78.1(3)
\|$\Omega _{\rm in}$\|	4.1601	3.9969	3.8681	4.1601	3.8250	3.9108
\|$\Omega _{\rm out}$\|	3.5965	3.4406	3.3185	3.5965	3.2777	3.3588
\|$\Omega _{1}=\Omega _{2}$\|	4.0399(59)	4.0782(66)	3.7611(575)	4.0383(131)	3.7455(218)	3.8196(116)
\|$T_{2}\ (K)$\|	3895(5)	3894(15)	3917(17)	4104(6)	4111(3)	4126(3)
\|$L_{1}/(L_{1}+L_{2}+L_{3}$\|⁠) (B)	55.14\|$\%$\|	56.68\|$\%$\|	...	54.50\|$\%$\|	58.05\|$\%$\|	...
\|$L_{1}/(L_{1}+L_{2}+L_{3}$\|⁠) (V)	53.30\|$\%$\|	55.00\|$\%$\|	55.72\|$\%$\|	52.70\|$\%$\|	56.54\|$\%$\|	54.98\|$\%$\|
\|$L_{1}/(L_{1}+L_{2}+L_{3}$\|⁠) (R)	51.93\|$\%$\|	53.39\|$\%$\|	54.24\|$\%$\|	51.41\|$\%$\|	54.91\|$\%$\|	53.48\|$\%$\|
\|$L_{1}/(L_{1}+L_{2}+L_{3}$\|⁠) (I)	49.75\|$\%$\|	50.82\|$\%$\|	51.76\|$\%$\|	49.40\|$\%$\|	52.45\|$\%$\|	50.73\|$\%$\|
\|$L_{3}/(L_{1}+L_{2}+L_{3}$\|⁠) (B)	1.4(0.6)\|$\%$\|	1.8(1.5)\|$\%$\|	2.5(1.5)\|$\%$\|	2.9(0.5)\|$\%$\|	...
\|$L_{3}/(L_{1}+L_{2}+L_{3}$\|⁠) (V)	1.9(0.7)\|$\%$\|	1.8(1.5)\|$\%$\|	2.6(1.9)\|$\%$\|	2.7(0.6)\|$\%$\|	2.0(1.1)\|$\%$\|	2.3(0.5)\|$\%$\|
\|$L_{3}/(L_{1}+L_{2}+L_{3}$\|⁠) (R)	2.6(0.6)\|$\%$\|	3.1(1.4)\|$\%$\|	3.9(1.9)\|$\%$\|	3.2(0.5)\|$\%$\|	2.5(1.2)\|$\%$\|	2.8(0.3)\|$\%$\|
\|$L_{3}/(L_{1}+L_{2}+L_{3}$\|⁠) (I)	3.4(0.6)\|$\%$\|	4.6(1.4)\|$\%$\|	5.6(1.8)\|$\%$\|	4.8(0.3)\|$\%$\|	4.1(1.1)\|$\%$\|	4.2(0.5)\|$\%$\|
\|$r_{1}$\| (pole)	0.3509(7)	0.3569(19)	0.3636(32)	0.3510(15)	0.3637(14)	0.3591(10)
\|$r_{1}$\| (side)	0.3700(9)	0.3765(21)	0.3841(36)	0.3702(19)	0.3839(17)	0.3786(11)
\|$r_{1}$\| (back)	0.4101(14)	0.4153(24)	0.4329(38)	0.4103(29)	0.4220(21)	0.4154(11)
\|$r_{2}$\| (pole)	0.3891(7)	0.3825(64)	0.3747(111)	0.3893(15)	0.3736(41)	0.3725(35)
\|$r_{2}$\| (side)	0.4127(8)	0.4052(82)	0.3962(142)	0.4129(19)	0.3950(53)	0.3934(44)
\|$r_{2}$\| (back)	0.4497(13)	0.4431(13)	0.4335(227)	0.4490(28)	0.4325(83)	0.4287(69)
f	21.1(1.4)\|$\%$\|	21.0(6.3)\|$\%$\|	19.5(10.5)\|$\%$\|	21.6(2.3)\|$\%$\|	18.7(3.9)\|$\%$\|	16.5(2.1)\|$\%$\|
\|$\Sigma$\| res\|$^{2}$\|	0.0298	0.0116	0.0122	0.0104	0.0010	0.0111

This Feature Is Available To Subscribers Only