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 |
|---|---|---|---|---|---|---|---|---|---|
| 3850 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{3}M_{5}$ + ${ }\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{4}X_{1}$ + ${ }M_{6}\phi_{1}q_{1}^{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{7}q_{2}\tilde{q}_{1}$ | 0.667 | 0.8406 | 0.7935 | [X:[1.6116], M:[0.8348, 0.7187, 1.1652, 0.3884, 0.8348, 0.8058, 0.8058], q:[0.4029, 0.7623], qb:[0.4319, 0.8493], phi:[0.3884]] | [X:[[4]], M:[[12], [-28], [-12], [-4], [12], [2], [2]], q:[[1], [-13]], qb:[[11], [17]], phi:[[-4]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{6}$, ${ }M_{7}$, ${ }M_{1}$, ${ }M_{5}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{2}M_{6}$, ${ }M_{2}M_{7}$, ${ }M_{1}M_{2}$, ${ }M_{2}M_{5}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{6}^{2}$, ${ }M_{6}M_{7}$, ${ }M_{7}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }X_{1}$, ${ }M_{1}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{1}M_{7}$, ${ }M_{5}M_{7}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{5}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ | ${}\phi_{1}^{3}q_{1}\tilde{q}_{1}$ | -2 | t^2.156 + t^2.33 + 2*t^2.417 + 2*t^2.504 + t^3.67 + 2*t^3.757 + t^4.312 + t^4.487 + 2*t^4.574 + 3*t^4.661 + 2*t^4.748 + 6*t^4.835 + 4*t^4.922 + 3*t^5.009 - 2*t^6. + 2*t^6.087 + 5*t^6.174 + 4*t^6.261 + t^6.469 + t^6.643 + 2*t^6.73 + 3*t^6.817 + 2*t^6.904 + 6*t^6.991 + 4*t^7.078 + 6*t^7.165 + 6*t^7.252 + 8*t^7.339 + 6*t^7.426 + 6*t^7.513 - 3*t^8.156 - 2*t^8.243 - 3*t^8.33 - 6*t^8.417 - 3*t^8.504 + 8*t^8.592 + t^8.625 + 8*t^8.679 + 6*t^8.766 + t^8.799 + 2*t^8.886 + 3*t^8.973 - t^4.165/y - t^6.321/y - t^6.496/y - (2*t^6.583)/y - t^6.67/y + t^7.487/y + (2*t^7.574)/y + (3*t^7.661)/y + (4*t^7.748)/y + (4*t^7.835)/y + (4*t^7.922)/y + (2*t^8.009)/y - t^8.478/y - t^8.652/y - (2*t^8.739)/y - t^8.826/y - t^4.165*y - t^6.321*y - t^6.496*y - 2*t^6.583*y - t^6.67*y + t^7.487*y + 2*t^7.574*y + 3*t^7.661*y + 4*t^7.748*y + 4*t^7.835*y + 4*t^7.922*y + 2*t^8.009*y - t^8.478*y - t^8.652*y - 2*t^8.739*y - t^8.826*y | t^2.156/g1^28 + t^2.33/g1^8 + 2*g1^2*t^2.417 + 2*g1^12*t^2.504 + g1^8*t^3.67 + 2*g1^18*t^3.757 + t^4.312/g1^56 + t^4.487/g1^36 + (2*t^4.574)/g1^26 + (3*t^4.661)/g1^16 + (2*t^4.748)/g1^6 + 6*g1^4*t^4.835 + 4*g1^14*t^4.922 + 3*g1^24*t^5.009 - 2*t^6. + 2*g1^10*t^6.087 + 5*g1^20*t^6.174 + 4*g1^30*t^6.261 + t^6.469/g1^84 + t^6.643/g1^64 + (2*t^6.73)/g1^54 + (3*t^6.817)/g1^44 + (2*t^6.904)/g1^34 + (6*t^6.991)/g1^24 + (4*t^7.078)/g1^14 + (6*t^7.165)/g1^4 + 6*g1^6*t^7.252 + 8*g1^16*t^7.339 + 6*g1^26*t^7.426 + 6*g1^36*t^7.513 - (3*t^8.156)/g1^28 - (2*t^8.243)/g1^18 - (3*t^8.33)/g1^8 - 6*g1^2*t^8.417 - 3*g1^12*t^8.504 + 8*g1^22*t^8.592 + t^8.625/g1^112 + 8*g1^32*t^8.679 + 6*g1^42*t^8.766 + t^8.799/g1^92 + (2*t^8.886)/g1^82 + (3*t^8.973)/g1^72 - t^4.165/(g1^4*y) - t^6.321/(g1^32*y) - t^6.496/(g1^12*y) - (2*t^6.583)/(g1^2*y) - (g1^8*t^6.67)/y + t^7.487/(g1^36*y) + (2*t^7.574)/(g1^26*y) + (3*t^7.661)/(g1^16*y) + (4*t^7.748)/(g1^6*y) + (4*g1^4*t^7.835)/y + (4*g1^14*t^7.922)/y + (2*g1^24*t^8.009)/y - t^8.478/(g1^60*y) - t^8.652/(g1^40*y) - (2*t^8.739)/(g1^30*y) - t^8.826/(g1^20*y) - (t^4.165*y)/g1^4 - (t^6.321*y)/g1^32 - (t^6.496*y)/g1^12 - (2*t^6.583*y)/g1^2 - g1^8*t^6.67*y + (t^7.487*y)/g1^36 + (2*t^7.574*y)/g1^26 + (3*t^7.661*y)/g1^16 + (4*t^7.748*y)/g1^6 + 4*g1^4*t^7.835*y + 4*g1^14*t^7.922*y + 2*g1^24*t^8.009*y - (t^8.478*y)/g1^60 - (t^8.652*y)/g1^40 - (2*t^8.739*y)/g1^30 - (t^8.826*y)/g1^20 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 3374 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{3}M_{5}$ + ${ }\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{4}X_{1}$ + ${ }M_{6}\phi_{1}q_{1}^{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ | 0.6509 | 0.8123 | 0.8013 | [X:[1.6121], M:[0.8363, 0.7152, 1.1637, 0.3879, 0.8363, 0.8061], q:[0.403, 0.7606], qb:[0.4333, 0.8515], phi:[0.3879]] | t^2.146 + t^2.327 + t^2.418 + 2*t^2.509 + t^3.582 + t^3.673 + 2*t^3.764 + t^4.291 + t^4.473 + t^4.564 + 3*t^4.655 + t^4.745 + 4*t^4.836 + 2*t^4.927 + 3*t^5.018 + t^5.727 + t^5.909 - t^6. - t^4.164/y - t^4.164*y | detail |