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 |
|---|---|---|---|---|---|---|---|---|---|
| 4634 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{6}\phi_{1}^{2}$ + ${ }M_{4}M_{7}$ + ${ }M_{3}M_{8}$ | 0.6914 | 0.848 | 0.8153 | [M:[1.0025, 0.9992, 0.9975, 1.0042, 0.9958, 0.9992, 0.9958, 1.0025], q:[0.4979, 0.4996], qb:[0.5047, 0.4962], phi:[0.5004]] | [M:[[-6], [2], [6], [-10], [10], [2], [10], [-6]], q:[[5], [1]], qb:[[-11], [9]], phi:[[-1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}q_{1}\tilde{q}_{2}$, ${ }M_{5}$, ${ }M_{7}$, ${ }M_{2}$, ${ }M_{6}$, ${ }M_{1}$, ${ }M_{8}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }M_{5}q_{1}\tilde{q}_{2}$, ${ }M_{7}q_{1}\tilde{q}_{2}$, ${ }M_{5}^{2}$, ${ }M_{5}M_{7}$, ${ }M_{7}^{2}$, ${ }M_{6}q_{1}\tilde{q}_{2}$, ${ }M_{2}M_{5}$, ${ }M_{5}M_{6}$, ${ }M_{2}M_{7}$, ${ }M_{6}M_{7}$, ${ }M_{8}q_{1}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{2}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{1}M_{7}$, ${ }M_{5}M_{8}$, ${ }M_{7}M_{8}$ | ${}$ | -4 | t^2.982 + 2*t^2.987 + 2*t^2.997 + 2*t^3.008 + t^4.478 + t^4.483 + 2*t^4.489 + t^4.494 + t^4.499 + t^4.504 + t^4.509 + t^4.514 + t^4.529 + t^5.964 + 2*t^5.969 + 2*t^5.975 + t^5.98 + 3*t^5.985 + t^5.99 + 4*t^5.995 - 4*t^6. + 2*t^6.005 - t^6.01 + 2*t^6.015 - t^6.02 - t^6.025 + t^7.461 + 3*t^7.466 + 3*t^7.471 + 4*t^7.476 + 2*t^7.481 + 5*t^7.486 + 3*t^7.491 + 3*t^7.496 + 2*t^7.511 + 2*t^7.517 + 2*t^7.537 + t^8.947 + 2*t^8.952 + 3*t^8.957 + 4*t^8.962 + 4*t^8.967 + 6*t^8.972 + 3*t^8.977 + 2*t^8.982 - 5*t^8.987 + 4*t^8.992 - 5*t^8.997 - t^4.501/y - t^7.489/y + t^7.494/y - t^7.499/y + t^7.504/y - t^7.509/y + t^7.514/y + (2*t^8.969)/y + t^8.975/y + (2*t^8.98)/y + (4*t^8.985)/y + (2*t^8.99)/y + (5*t^8.995)/y - t^4.501*y - t^7.489*y + t^7.494*y - t^7.499*y + t^7.504*y - t^7.509*y + t^7.514*y + 2*t^8.969*y + t^8.975*y + 2*t^8.98*y + 4*t^8.985*y + 2*t^8.99*y + 5*t^8.995*y | g1^14*t^2.982 + 2*g1^10*t^2.987 + 2*g1^2*t^2.997 + (2*t^3.008)/g1^6 + g1^17*t^4.478 + g1^13*t^4.483 + 2*g1^9*t^4.489 + g1^5*t^4.494 + g1*t^4.499 + t^4.504/g1^3 + t^4.509/g1^7 + t^4.514/g1^11 + t^4.529/g1^23 + g1^28*t^5.964 + 2*g1^24*t^5.969 + 2*g1^20*t^5.975 + g1^16*t^5.98 + 3*g1^12*t^5.985 + g1^8*t^5.99 + 4*g1^4*t^5.995 - 4*t^6. + (2*t^6.005)/g1^4 - t^6.01/g1^8 + (2*t^6.015)/g1^12 - t^6.02/g1^16 - t^6.025/g1^20 + g1^31*t^7.461 + 3*g1^27*t^7.466 + 3*g1^23*t^7.471 + 4*g1^19*t^7.476 + 2*g1^15*t^7.481 + 5*g1^11*t^7.486 + 3*g1^7*t^7.491 + 3*g1^3*t^7.496 + (2*t^7.511)/g1^9 + (2*t^7.517)/g1^13 + (2*t^7.537)/g1^29 + g1^42*t^8.947 + 2*g1^38*t^8.952 + 3*g1^34*t^8.957 + 4*g1^30*t^8.962 + 4*g1^26*t^8.967 + 6*g1^22*t^8.972 + 3*g1^18*t^8.977 + 2*g1^14*t^8.982 - 5*g1^10*t^8.987 + 4*g1^6*t^8.992 - 5*g1^2*t^8.997 - t^4.501/(g1*y) - (g1^9*t^7.489)/y + (g1^5*t^7.494)/y - (g1*t^7.499)/y + t^7.504/(g1^3*y) - t^7.509/(g1^7*y) + t^7.514/(g1^11*y) + (2*g1^24*t^8.969)/y + (g1^20*t^8.975)/y + (2*g1^16*t^8.98)/y + (4*g1^12*t^8.985)/y + (2*g1^8*t^8.99)/y + (5*g1^4*t^8.995)/y - (t^4.501*y)/g1 - g1^9*t^7.489*y + g1^5*t^7.494*y - g1*t^7.499*y + (t^7.504*y)/g1^3 - (t^7.509*y)/g1^7 + (t^7.514*y)/g1^11 + 2*g1^24*t^8.969*y + g1^20*t^8.975*y + 2*g1^16*t^8.98*y + 4*g1^12*t^8.985*y + 2*g1^8*t^8.99*y + 5*g1^4*t^8.995*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 |
|---|---|---|---|---|---|---|---|---|---|
| 2561 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{6}\phi_{1}^{2}$ + ${ }M_{4}M_{7}$ | 0.6921 | 0.8506 | 0.8137 | [M:[1.0113, 0.9962, 0.9887, 1.0188, 0.9812, 0.9962, 0.9812], q:[0.4906, 0.4981], qb:[0.5206, 0.4831], phi:[0.5019]] | t^2.921 + 2*t^2.944 + t^2.966 + 2*t^2.989 + t^3.034 + t^4.404 + t^4.427 + 2*t^4.449 + t^4.472 + t^4.494 + t^4.517 + t^4.539 + t^4.562 + t^4.629 + t^5.842 + 2*t^5.865 + 3*t^5.887 + 3*t^5.91 + 4*t^5.932 + 2*t^5.955 + 2*t^5.977 - 3*t^6. - t^4.506/y - t^4.506*y | detail |