Chosen Fixed Point
Here is the data for the chosen fixed point.
$F_{UV}$ represents the flavor symmetries in the UV Lagrangian, and $F_{IR}$ represents the flavor symmetries in the IR. $F_{UV}$ and $F_{IR}$ can differ due to accidental symmetry enhancement.
The number of marginal operators, $n_{marginal}$, minus the dimension of flavor symmetries in IR, $|F_{IR}|$, corresponds to the coefficient of $t^6$ in the superconformal index.
# | Theory | Superpotential | Central charge $a$ | Central charge $c$ | Ratio $a/c$ | Matter field: $R$-charge | U(1) part of $F_{UV}$ | Rank of $F_{UV}$ | Rational |
---|---|---|---|---|---|---|---|---|---|
419 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{1}M_{4}$ | 0.6483 | 0.7846 | 0.8263 | [M:[1.09, 1.09, 1.005, 0.91], q:[0.7725, 0.4125], qb:[0.4975, 0.4975], phi:[0.455]] | [M:[[4], [4], [-22], [-4]], q:[[1], [-15]], qb:[[11], [11]], phi:[[-2]]] | 1 |
Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
---|---|---|---|---|
${}M_{4}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{1}$, ${ }q_{1}q_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$ | ${}M_{1}\phi_{1}^{2}$ | -3 | 2*t^2.73 + t^3.015 + t^3.27 + t^3.555 + 2*t^3.81 + t^3.84 + 2*t^4.095 + 3*t^4.35 + 3*t^5.46 - 3*t^6. + t^6.03 - 2*t^6.255 + 2*t^6.285 + 2*t^6.54 + 3*t^6.57 + 4*t^6.825 + t^6.855 + 5*t^7.08 + t^7.11 + t^7.365 + t^7.395 + t^7.62 + 2*t^7.65 + t^7.68 + 3*t^7.905 + 2*t^7.935 + 4*t^8.16 + 6*t^8.19 + 2*t^8.445 - t^8.475 + 5*t^8.7 - 7*t^8.73 - 4*t^8.985 - t^4.365/y + t^7.35/y - t^7.38/y + t^8.46/y + (2*t^8.745)/y - t^4.365*y + t^7.35*y - t^7.38*y + t^8.46*y + 2*t^8.745*y | (2*t^2.73)/g1^4 + t^3.015/g1^22 + g1^4*t^3.27 + t^3.555/g1^14 + 2*g1^12*t^3.81 + t^3.84/g1^32 + (2*t^4.095)/g1^6 + 3*g1^20*t^4.35 + (3*t^5.46)/g1^8 - 3*t^6. + t^6.03/g1^44 - 2*g1^26*t^6.255 + (2*t^6.285)/g1^18 + 2*g1^8*t^6.54 + (3*t^6.57)/g1^36 + (4*t^6.825)/g1^10 + t^6.855/g1^54 + 5*g1^16*t^7.08 + t^7.11/g1^28 + t^7.365/g1^2 + t^7.395/g1^46 + g1^24*t^7.62 + (2*t^7.65)/g1^20 + t^7.68/g1^64 + 3*g1^6*t^7.905 + (2*t^7.935)/g1^38 + 4*g1^32*t^8.16 + (6*t^8.19)/g1^12 + 2*g1^14*t^8.445 - t^8.475/g1^30 + 5*g1^40*t^8.7 - (7*t^8.73)/g1^4 - 4*g1^22*t^8.985 - t^4.365/(g1^2*y) + (g1^20*t^7.35)/y - t^7.38/(g1^24*y) + t^8.46/(g1^8*y) + (2*t^8.745)/(g1^26*y) - (t^4.365*y)/g1^2 + g1^20*t^7.35*y - (t^7.38*y)/g1^24 + (t^8.46*y)/g1^8 + (2*t^8.745*y)/g1^26 |
Deformation
Here is the data for the deformed fixed points from the chosen fixed point.
# | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
---|---|---|---|---|---|---|---|---|
693 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{1}M_{4}$ + ${ }M_{1}M_{5}$ | 0.6566 | 0.7988 | 0.822 | [M:[1.0916, 1.0916, 0.9962, 0.9084, 0.9084], q:[0.7729, 0.4065], qb:[0.5019, 0.5019], phi:[0.4542]] | 3*t^2.725 + t^2.989 + t^3.538 + t^3.802 + 2*t^3.824 + 2*t^4.088 + 3*t^4.374 + 6*t^5.45 + t^5.714 + t^5.977 - 5*t^6. - t^4.363/y - t^4.363*y | detail | |
691 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}\phi_{1}q_{2}^{2}$ | 0.6687 | 0.8234 | 0.8121 | [M:[1.0874, 1.0874, 1.0193, 0.9126, 0.6991], q:[0.7718, 0.4223], qb:[0.4903, 0.4903], phi:[0.4563]] | t^2.097 + 2*t^2.738 + t^3.058 + t^3.262 + t^3.582 + 2*t^3.787 + 2*t^4.107 + t^4.195 + 3*t^4.311 + 2*t^4.835 + t^5.155 + t^5.36 + 3*t^5.476 + t^5.68 + 2*t^5.884 - 3*t^6. - t^4.369/y - t^4.369*y | detail | |
694 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{2}M_{4}$ + ${ }M_{1}M_{4}$ + ${ }M_{5}q_{1}q_{2}$ | 0.6643 | 0.8125 | 0.8176 | [M:[1.086, 1.086, 1.0269, 0.914, 0.8011], q:[0.7715, 0.4274], qb:[0.4866, 0.4866], phi:[0.457]] | t^2.403 + 2*t^2.742 + t^3.081 + t^3.258 + 2*t^3.774 + t^3.935 + 2*t^4.113 + 3*t^4.29 + t^4.806 + 2*t^5.145 + 4*t^5.484 + t^5.661 - 3*t^6. - t^4.371/y - t^4.371*y | detail |
Equivalent Fixed Points from Other Seed Theories
Here is a list of equivalent fixed points from other gauge theories.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
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Equivalent Fixed Points from the Same Seed Theory
Below is a list of equivalent fixed points from the same seed theories.
id | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | More Info. | Rational |
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Previous Theory
The previous fixed point before deforming to get the chosen fixed point.
# | Theory | Superpotential | Central Charge $a$ | Central Charge $c$ | Ratio $a/c$ | $R$-charges | Superconformal Index | More Info. | Rational |
---|---|---|---|---|---|---|---|---|---|
264 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{2}M_{4}$ | 0.6607 | 0.8017 | 0.8242 | [M:[0.9624, 1.1278, 0.9624, 0.8722], q:[0.782, 0.4361], qb:[0.6015, 0.4361], phi:[0.4361]] | 2*t^2.617 + 2*t^2.887 + 2*t^3.654 + 3*t^3.925 + t^4.15 + 2*t^4.421 + t^4.917 + 3*t^5.233 + 2*t^5.504 + 3*t^5.774 - 5*t^6. - t^4.308/y - t^4.308*y | detail |