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 |
|---|---|---|---|---|---|---|---|---|---|
| 55200 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{5}$ + ${ }M_{4}\phi_{1}q_{1}^{2}$ + ${ }M_{6}\phi_{1}q_{1}q_{2}$ | 0.6679 | 0.8411 | 0.7941 | [M:[1.1573, 0.736, 0.8427, 0.8071, 0.8427, 0.7715], q:[0.4036, 0.4391], qb:[0.8605, 0.7538], phi:[0.3858]] | [M:[[12], [18], [-12], [-2], [-12], [8]], q:[[-1], [-11]], qb:[[-17], [13]], phi:[[4]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{4}$, ${ }M_{3}$, ${ }M_{5}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{6}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}M_{3}$, ${ }M_{2}M_{5}$, ${ }M_{4}M_{6}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}M_{5}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{5}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$ | ${}M_{2}\phi_{1}q_{2}^{2}$ | -1 | t^2.208 + 2*t^2.315 + t^2.421 + 2*t^2.528 + t^3.579 + t^3.792 + t^3.899 + t^4.416 + 2*t^4.523 + 4*t^4.629 + 4*t^4.736 + 6*t^4.843 + 2*t^4.949 + 3*t^5.056 - t^6. + 3*t^6.107 + 2*t^6.213 + 3*t^6.32 + 2*t^6.427 + t^6.624 + 2*t^6.73 + 4*t^6.837 + 7*t^6.944 + 7*t^7.051 + 10*t^7.157 + 5*t^7.264 + 7*t^7.371 + 2*t^7.477 + 4*t^7.584 + t^7.691 + t^7.798 - 2*t^8.101 - 3*t^8.208 - 5*t^8.315 - 2*t^8.421 - 2*t^8.528 + 6*t^8.635 + 5*t^8.742 + t^8.832 + 5*t^8.848 + 2*t^8.938 + 3*t^8.955 - t^4.157/y - t^6.365/y - (2*t^6.472)/y - t^6.579/y - t^6.685/y + (2*t^7.523)/y + (3*t^7.629)/y + (5*t^7.736)/y + (6*t^7.843)/y + (3*t^7.949)/y + t^8.056/y - t^8.573/y - (2*t^8.68)/y - (3*t^8.787)/y - t^8.893/y - t^4.157*y - t^6.365*y - 2*t^6.472*y - t^6.579*y - t^6.685*y + 2*t^7.523*y + 3*t^7.629*y + 5*t^7.736*y + 6*t^7.843*y + 3*t^7.949*y + t^8.056*y - t^8.573*y - 2*t^8.68*y - 3*t^8.787*y - t^8.893*y | g1^18*t^2.208 + 2*g1^8*t^2.315 + t^2.421/g1^2 + (2*t^2.528)/g1^12 + g1^2*t^3.579 + t^3.792/g1^18 + t^3.899/g1^28 + g1^36*t^4.416 + 2*g1^26*t^4.523 + 4*g1^16*t^4.629 + 4*g1^6*t^4.736 + (6*t^4.843)/g1^4 + (2*t^4.949)/g1^14 + (3*t^5.056)/g1^24 - t^6. + (3*t^6.107)/g1^10 + (2*t^6.213)/g1^20 + (3*t^6.32)/g1^30 + (2*t^6.427)/g1^40 + g1^54*t^6.624 + 2*g1^44*t^6.73 + 4*g1^34*t^6.837 + 7*g1^24*t^6.944 + 7*g1^14*t^7.051 + 10*g1^4*t^7.157 + (5*t^7.264)/g1^6 + (7*t^7.371)/g1^16 + (2*t^7.477)/g1^26 + (4*t^7.584)/g1^36 + t^7.691/g1^46 + t^7.798/g1^56 - 2*g1^28*t^8.101 - 3*g1^18*t^8.208 - 5*g1^8*t^8.315 - (2*t^8.421)/g1^2 - (2*t^8.528)/g1^12 + (6*t^8.635)/g1^22 + (5*t^8.742)/g1^32 + g1^72*t^8.832 + (5*t^8.848)/g1^42 + 2*g1^62*t^8.938 + (3*t^8.955)/g1^52 - (g1^4*t^4.157)/y - (g1^22*t^6.365)/y - (2*g1^12*t^6.472)/y - (g1^2*t^6.579)/y - t^6.685/(g1^8*y) + (2*g1^26*t^7.523)/y + (3*g1^16*t^7.629)/y + (5*g1^6*t^7.736)/y + (6*t^7.843)/(g1^4*y) + (3*t^7.949)/(g1^14*y) + t^8.056/(g1^24*y) - (g1^40*t^8.573)/y - (2*g1^30*t^8.68)/y - (3*g1^20*t^8.787)/y - (g1^10*t^8.893)/y - g1^4*t^4.157*y - g1^22*t^6.365*y - 2*g1^12*t^6.472*y - g1^2*t^6.579*y - (t^6.685*y)/g1^8 + 2*g1^26*t^7.523*y + 3*g1^16*t^7.629*y + 5*g1^6*t^7.736*y + (6*t^7.843*y)/g1^4 + (3*t^7.949*y)/g1^14 + (t^8.056*y)/g1^24 - g1^40*t^8.573*y - 2*g1^30*t^8.68*y - 3*g1^20*t^8.787*y - g1^10*t^8.893*y |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 47037 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{1}M_{5}$ + ${ }M_{4}\phi_{1}q_{1}^{2}$ | 0.6499 | 0.8094 | 0.803 | [M:[1.1637, 0.7456, 0.8363, 0.806, 0.8363], q:[0.403, 0.4332], qb:[0.8514, 0.7607], phi:[0.3879]] | t^2.237 + t^2.327 + t^2.418 + 2*t^2.509 + t^3.582 + t^3.673 + t^3.763 + t^3.854 + t^4.474 + t^4.564 + 2*t^4.655 + 3*t^4.746 + 4*t^4.836 + 2*t^4.927 + 3*t^5.018 - t^4.164/y - t^4.164*y | detail |