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 |
|---|---|---|---|---|---|---|---|---|---|
| 2790 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ | 0.6436 | 0.8453 | 0.7614 | [M:[0.9915, 1.0255, 0.7479, 0.7649, 0.7649], q:[0.7479, 0.2606], qb:[0.4872, 0.4872], phi:[0.5043]] | [M:[[4], [-12], [1], [-7], [-7]], q:[[1], [-5]], qb:[[6], [6]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{3}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{4}$, ${ }M_{5}$, ${ }M_{1}$, ${ }\phi_{1}^{2}$, ${ }M_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{3}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{3}M_{5}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }M_{5}q_{2}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{1}M_{3}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{5}$, ${ }M_{3}\phi_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{3}\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{2}$, ${ }M_{2}M_{4}$, ${ }M_{2}M_{5}$, ${ }M_{4}\phi_{1}q_{2}^{2}$, ${ }M_{5}\phi_{1}q_{2}^{2}$ | ${}\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$ | -2 | 3*t^2.244 + 2*t^2.295 + t^2.974 + t^3.026 + 2*t^3.077 + t^3.756 + 3*t^4.436 + 6*t^4.487 + 6*t^4.538 + 3*t^4.589 + 3*t^5.218 + 5*t^5.269 + 6*t^5.32 + 4*t^5.371 - 2*t^6. + 3*t^6.051 + 2*t^6.102 + 3*t^6.153 + 5*t^6.68 + 13*t^6.731 + 9*t^6.782 + 9*t^6.833 + 4*t^6.884 + 4*t^7.462 + 11*t^7.513 + 15*t^7.564 + 11*t^7.615 + 6*t^7.666 - 2*t^8.142 - 3*t^8.193 - 9*t^8.244 - 3*t^8.295 + 9*t^8.346 + 9*t^8.397 + 6*t^8.448 + 5*t^8.872 + 6*t^8.923 + 11*t^8.974 - t^4.513/y - t^6.756/y - (2*t^6.807)/y + t^7.436/y + (3*t^7.487)/y + (6*t^7.538)/y + (5*t^8.218)/y + (6*t^8.269)/y + (8*t^8.32)/y + (4*t^8.371)/y - t^4.513*y - t^6.756*y - 2*t^6.807*y + t^7.436*y + 3*t^7.487*y + 6*t^7.538*y + 5*t^8.218*y + 6*t^8.269*y + 8*t^8.32*y + 4*t^8.371*y | 3*g1*t^2.244 + (2*t^2.295)/g1^7 + g1^4*t^2.974 + t^3.026/g1^4 + (2*t^3.077)/g1^12 + t^3.756/g1 + 3*g1^10*t^4.436 + 6*g1^2*t^4.487 + (6*t^4.538)/g1^6 + (3*t^4.589)/g1^14 + 3*g1^5*t^5.218 + (5*t^5.269)/g1^3 + (6*t^5.32)/g1^11 + (4*t^5.371)/g1^19 - 2*t^6. + (3*t^6.051)/g1^8 + (2*t^6.102)/g1^16 + (3*t^6.153)/g1^24 + 5*g1^11*t^6.68 + 13*g1^3*t^6.731 + (9*t^6.782)/g1^5 + (9*t^6.833)/g1^13 + (4*t^6.884)/g1^21 + 4*g1^6*t^7.462 + (11*t^7.513)/g1^2 + (15*t^7.564)/g1^10 + (11*t^7.615)/g1^18 + (6*t^7.666)/g1^26 - 2*g1^17*t^8.142 - 3*g1^9*t^8.193 - 9*g1*t^8.244 - (3*t^8.295)/g1^7 + (9*t^8.346)/g1^15 + (9*t^8.397)/g1^23 + (6*t^8.448)/g1^31 + 5*g1^20*t^8.872 + 6*g1^12*t^8.923 + 11*g1^4*t^8.974 - t^4.513/(g1^2*y) - t^6.756/(g1*y) - (2*t^6.807)/(g1^9*y) + (g1^10*t^7.436)/y + (3*g1^2*t^7.487)/y + (6*t^7.538)/(g1^6*y) + (5*g1^5*t^8.218)/y + (6*t^8.269)/(g1^3*y) + (8*t^8.32)/(g1^11*y) + (4*t^8.371)/(g1^19*y) - (t^4.513*y)/g1^2 - (t^6.756*y)/g1 - (2*t^6.807*y)/g1^9 + g1^10*t^7.436*y + 3*g1^2*t^7.487*y + (6*t^7.538*y)/g1^6 + 5*g1^5*t^8.218*y + (6*t^8.269*y)/g1^3 + (8*t^8.32*y)/g1^11 + (4*t^8.371*y)/g1^19 |
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 |
|---|
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 |
|---|
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 |
|---|
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 |
|---|---|---|---|---|---|---|---|---|---|
| 1782 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{3}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{4}q_{1}\tilde{q}_{1}$ | 0.6255 | 0.812 | 0.7702 | [M:[0.9852, 1.0444, 0.7463, 0.7759], q:[0.7463, 0.2685], qb:[0.4778, 0.4778], phi:[0.5074]] | 3*t^2.239 + t^2.328 + t^2.956 + t^3.044 + 2*t^3.133 + t^3.672 + t^3.761 + 3*t^4.389 + 6*t^4.478 + 3*t^4.567 + t^4.655 + 3*t^5.195 + 4*t^5.283 + 5*t^5.372 + 2*t^5.461 + 3*t^5.911 - t^6. - t^4.522/y - t^4.522*y | detail |