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 |
|---|---|---|---|---|---|---|---|---|---|
| 58900 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}q_{2}$ + ${ }M_{5}\phi_{1}q_{1}^{2}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ + ${ }M_{7}\phi_{1}^{2}$ + ${ }M_{8}\phi_{1}q_{1}^{2}$ | 0.7103 | 0.9129 | 0.778 | [M:[1.1789, 1.0318, 0.8211, 0.8211, 0.7157, 0.7157, 1.0735, 0.7157], q:[0.4105, 0.4105], qb:[0.5576, 0.7684], phi:[0.4632]] | [M:[[2], [-22], [-2], [-2], [8], [8], [12], [8]], q:[[-1], [-1]], qb:[[23], [3]], phi:[[-6]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{5}$, ${ }M_{6}$, ${ }M_{8}$, ${ }M_{3}$, ${ }M_{4}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{2}$, ${ }M_{7}$, ${ }M_{1}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}^{2}$, ${ }M_{5}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{5}M_{8}$, ${ }M_{6}M_{8}$, ${ }M_{8}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{3}M_{5}$, ${ }M_{4}M_{5}$, ${ }M_{3}M_{6}$, ${ }M_{4}M_{6}$, ${ }M_{3}M_{8}$, ${ }M_{4}M_{8}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }M_{6}q_{2}\tilde{q}_{1}$, ${ }M_{8}q_{2}\tilde{q}_{1}$, ${ }M_{2}M_{5}$, ${ }M_{2}M_{6}$, ${ }M_{2}M_{8}$, ${ }M_{5}M_{7}$, ${ }M_{6}M_{7}$, ${ }M_{7}M_{8}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}M_{5}$, ${ }M_{1}M_{6}$, ${ }M_{3}M_{7}$, ${ }M_{4}M_{7}$, ${ }M_{1}M_{8}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$ | ${}M_{1}M_{4}$, ${ }M_{2}q_{2}\tilde{q}_{1}$ | -2 | 3*t^2.147 + 2*t^2.463 + t^2.904 + t^3.096 + t^3.221 + t^3.537 + t^3.978 + 8*t^4.294 + 6*t^4.61 + t^4.735 + 3*t^4.926 + 3*t^5.052 + 3*t^5.243 + 5*t^5.368 + 5*t^5.684 + t^5.809 - 2*t^6. + 4*t^6.125 + t^6.191 - t^6.316 + 17*t^6.441 + 14*t^6.757 + 4*t^6.882 - 2*t^6.948 + 6*t^7.074 + 10*t^7.199 + 6*t^7.39 + 13*t^7.515 + t^7.64 - t^7.706 + 12*t^7.831 + 4*t^7.956 - t^8.022 - 7*t^8.147 + 12*t^8.272 + 3*t^8.338 - 10*t^8.463 + 31*t^8.588 + t^8.654 + 2*t^8.713 - 4*t^8.779 + 23*t^8.904 - t^4.39/y - (3*t^6.537)/y - t^6.853/y + (4*t^7.294)/y - t^7.485/y + (6*t^7.61)/y + (2*t^7.926)/y + (3*t^8.052)/y + (6*t^8.243)/y + (5*t^8.368)/y + (2*t^8.559)/y - t^8.684/y - t^4.39*y - 3*t^6.537*y - t^6.853*y + 4*t^7.294*y - t^7.485*y + 6*t^7.61*y + 2*t^7.926*y + 3*t^8.052*y + 6*t^8.243*y + 5*t^8.368*y + 2*t^8.559*y - t^8.684*y | 3*g1^8*t^2.147 + (2*t^2.463)/g1^2 + g1^22*t^2.904 + t^3.096/g1^22 + g1^12*t^3.221 + g1^2*t^3.537 + g1^26*t^3.978 + 8*g1^16*t^4.294 + 6*g1^6*t^4.61 + g1^40*t^4.735 + (3*t^4.926)/g1^4 + 3*g1^30*t^5.052 + (3*t^5.243)/g1^14 + 5*g1^20*t^5.368 + 5*g1^10*t^5.684 + g1^44*t^5.809 - 2*t^6. + 4*g1^34*t^6.125 + t^6.191/g1^44 - t^6.316/g1^10 + 17*g1^24*t^6.441 + 14*g1^14*t^6.757 + 4*g1^48*t^6.882 - (2*t^6.948)/g1^30 + 6*g1^4*t^7.074 + 10*g1^38*t^7.199 + (6*t^7.39)/g1^6 + 13*g1^28*t^7.515 + g1^62*t^7.64 - t^7.706/g1^16 + 12*g1^18*t^7.831 + 4*g1^52*t^7.956 - t^8.022/g1^26 - 7*g1^8*t^8.147 + 12*g1^42*t^8.272 + (3*t^8.338)/g1^36 - (10*t^8.463)/g1^2 + 31*g1^32*t^8.588 + t^8.654/g1^46 + 2*g1^66*t^8.713 - (4*t^8.779)/g1^12 + 23*g1^22*t^8.904 - t^4.39/(g1^6*y) - (3*g1^2*t^6.537)/y - t^6.853/(g1^8*y) + (4*g1^16*t^7.294)/y - t^7.485/(g1^28*y) + (6*g1^6*t^7.61)/y + (2*t^7.926)/(g1^4*y) + (3*g1^30*t^8.052)/y + (6*t^8.243)/(g1^14*y) + (5*g1^20*t^8.368)/y + (2*t^8.559)/(g1^24*y) - (g1^10*t^8.684)/y - (t^4.39*y)/g1^6 - 3*g1^2*t^6.537*y - (t^6.853*y)/g1^8 + 4*g1^16*t^7.294*y - (t^7.485*y)/g1^28 + 6*g1^6*t^7.61*y + (2*t^7.926*y)/g1^4 + 3*g1^30*t^8.052*y + (6*t^8.243*y)/g1^14 + 5*g1^20*t^8.368*y + (2*t^8.559*y)/g1^24 - g1^10*t^8.684*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 |
|---|---|---|---|---|---|---|---|---|---|
| 56618 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}q_{2}$ + ${ }M_{5}\phi_{1}q_{1}^{2}$ + ${ }M_{6}\phi_{1}q_{2}^{2}$ + ${ }M_{7}\phi_{1}^{2}$ | 0.6901 | 0.8745 | 0.7891 | [M:[1.1794, 1.0269, 0.8206, 0.8206, 0.7175, 0.7175, 1.0762], q:[0.4103, 0.4103], qb:[0.5628, 0.7691], phi:[0.4619]] | 2*t^2.152 + 2*t^2.462 + t^2.919 + t^3.081 + t^3.229 + t^3.538 + t^3.848 + t^3.995 + 5*t^4.305 + 4*t^4.614 + t^4.762 + 3*t^4.924 + 2*t^5.072 + 2*t^5.233 + 4*t^5.381 + 4*t^5.691 + t^5.838 - t^4.386/y - t^4.386*y | detail |