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 |
|---|---|---|---|---|---|---|---|---|---|
| 6164 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{7}$ + ${ }M_{8}\phi_{1}^{2}$ + ${ }M_{5}M_{9}$ | 0.6889 | 0.8465 | 0.8139 | [M:[1.0798, 0.7606, 0.9015, 0.9389, 1.0611, 0.7793, 1.2394, 1.0798, 0.9389], q:[0.5399, 0.3803], qb:[0.5586, 0.6808], phi:[0.4601]] | [M:[[-2], [6], [15], [-11], [11], [-7], [-6], [-2], [-11]], q:[[-1], [3]], qb:[[-14], [8]], phi:[[1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{6}$, ${ }M_{3}$, ${ }M_{4}$, ${ }M_{9}$, ${ }M_{1}$, ${ }M_{8}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{7}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}M_{6}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}M_{9}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{3}M_{9}$, ${ }M_{1}M_{6}$, ${ }M_{6}M_{8}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{9}$, ${ }M_{9}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{3}M_{8}$ | ${}$ | -3 | t^2.338 + t^2.705 + 2*t^2.817 + 2*t^3.239 + t^3.662 + t^3.718 + t^4.141 + t^4.197 + t^4.564 + t^4.62 + 2*t^4.676 + t^4.732 + 2*t^5.042 + 2*t^5.154 + t^5.409 + t^5.521 + t^5.577 + 2*t^5.633 + t^5.944 - 3*t^6. + 4*t^6.056 + 3*t^6.479 + 2*t^6.535 + t^6.902 + 3*t^6.958 + 3*t^7.014 + t^7.07 + t^7.268 + 3*t^7.38 + 3*t^7.436 + 3*t^7.492 + 2*t^7.548 + t^7.747 + 2*t^7.859 + 2*t^7.915 + 3*t^7.971 + t^8.114 + t^8.226 + 2*t^8.282 - 2*t^8.338 + 4*t^8.394 + 3*t^8.45 + 2*t^8.649 - 3*t^8.705 + 2*t^8.761 - 4*t^8.817 + 5*t^8.873 + t^8.929 - t^4.38/y - t^6.718/y - t^7.085/y + t^7.141/y - t^7.197/y + t^7.564/y - t^7.62/y + t^7.676/y + (2*t^8.042)/y + (2*t^8.154)/y + (2*t^8.521)/y + (2*t^8.577)/y + t^8.633/y + (2*t^8.944)/y - t^4.38*y - t^6.718*y - t^7.085*y + t^7.141*y - t^7.197*y + t^7.564*y - t^7.62*y + t^7.676*y + 2*t^8.042*y + 2*t^8.154*y + 2*t^8.521*y + 2*t^8.577*y + t^8.633*y + 2*t^8.944*y | t^2.338/g1^7 + g1^15*t^2.705 + (2*t^2.817)/g1^11 + (2*t^3.239)/g1^2 + g1^7*t^3.662 + t^3.718/g1^6 + g1^3*t^4.141 + t^4.197/g1^10 + g1^12*t^4.564 + t^4.62/g1 + (2*t^4.676)/g1^14 + t^4.732/g1^27 + 2*g1^8*t^5.042 + (2*t^5.154)/g1^18 + g1^30*t^5.409 + g1^4*t^5.521 + t^5.577/g1^9 + (2*t^5.633)/g1^22 + g1^13*t^5.944 - 3*t^6. + (4*t^6.056)/g1^13 + (3*t^6.479)/g1^4 + (2*t^6.535)/g1^17 + g1^5*t^6.902 + (3*t^6.958)/g1^8 + (3*t^7.014)/g1^21 + t^7.07/g1^34 + g1^27*t^7.268 + 3*g1*t^7.38 + (3*t^7.436)/g1^12 + (3*t^7.492)/g1^25 + (2*t^7.548)/g1^38 + g1^23*t^7.747 + (2*t^7.859)/g1^3 + (2*t^7.915)/g1^16 + (3*t^7.971)/g1^29 + g1^45*t^8.114 + g1^19*t^8.226 + 2*g1^6*t^8.282 - (2*t^8.338)/g1^7 + (4*t^8.394)/g1^20 + (3*t^8.45)/g1^33 + 2*g1^28*t^8.649 - 3*g1^15*t^8.705 + 2*g1^2*t^8.761 - (4*t^8.817)/g1^11 + (5*t^8.873)/g1^24 + t^8.929/g1^37 - (g1*t^4.38)/y - t^6.718/(g1^6*y) - (g1^16*t^7.085)/y + (g1^3*t^7.141)/y - t^7.197/(g1^10*y) + (g1^12*t^7.564)/y - t^7.62/(g1*y) + t^7.676/(g1^14*y) + (2*g1^8*t^8.042)/y + (2*t^8.154)/(g1^18*y) + (2*g1^4*t^8.521)/y + (2*t^8.577)/(g1^9*y) + t^8.633/(g1^22*y) + (2*g1^13*t^8.944)/y - g1*t^4.38*y - (t^6.718*y)/g1^6 - g1^16*t^7.085*y + g1^3*t^7.141*y - (t^7.197*y)/g1^10 + g1^12*t^7.564*y - (t^7.62*y)/g1 + (t^7.676*y)/g1^14 + 2*g1^8*t^8.042*y + (2*t^8.154*y)/g1^18 + 2*g1^4*t^8.521*y + (2*t^8.577*y)/g1^9 + (t^8.633*y)/g1^22 + 2*g1^13*t^8.944*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 |
|---|---|---|---|---|---|---|---|---|---|
| 4615 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{7}$ + ${ }M_{8}\phi_{1}^{2}$ | 0.6844 | 0.838 | 0.8167 | [M:[1.0844, 0.7469, 0.8673, 0.964, 1.036, 0.7953, 1.2531, 1.0844], q:[0.5422, 0.3735], qb:[0.5906, 0.6625], phi:[0.4578]] | t^2.386 + t^2.602 + t^2.892 + t^3.108 + 2*t^3.253 + t^3.614 + t^3.759 + t^4.12 + t^4.265 + t^4.481 + t^4.627 + 2*t^4.772 + t^4.917 + 2*t^4.988 + t^5.204 + t^5.278 + t^5.494 + t^5.639 + t^5.71 + t^5.855 - 2*t^6. - t^4.373/y - t^4.373*y | detail |