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 |
|---|---|---|---|---|---|---|---|---|---|
| 58550 | SU3adj1nf2 | ${}M_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ + ${ }q_{2}^{2}\tilde{q}_{2}^{2}$ + ${ }\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }q_{1}\tilde{q}_{2}X_{2}$ | 0.94 | 1.0838 | 0.8673 | [X:[1.3968, 1.508], M:[0.8096], q:[0.3915, 0.8995], qb:[0.7989, 0.1005], phi:[0.3016]] | [X:[[-6], [15]], M:[[18]], q:[[-16], [-1]], qb:[[-2], [1]], phi:[[3]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{1}$, ${ }\phi_{1}^{3}$, ${ }q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}\tilde{q}_{2}^{3}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }X_{1}$, ${ }X_{2}$, ${ }\phi_{1}^{2}q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{4}q_{1}\tilde{q}_{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{6}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{3}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$ | ${}\phi_{1}^{5}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{4}q_{1}\tilde{q}_{2}^{4}$ | 0 | t^2.38 + t^2.43 + t^2.71 + t^3. + t^3.29 + t^3.62 + t^3.9 + t^4.19 + t^4.52 + t^4.76 + t^4.81 + t^4.86 + 2*t^5.1 + t^5.14 + t^5.38 + 2*t^5.43 + t^5.67 + t^5.71 + t^5.95 + t^6.05 + t^6.24 + t^6.29 + t^6.33 + t^6.57 + 2*t^6.62 + 2*t^6.9 + t^6.95 + t^7.14 + 2*t^7.19 + 2*t^7.24 + t^7.29 + 2*t^7.48 + 2*t^7.52 + t^7.57 + t^7.76 + 4*t^7.81 + 2*t^7.86 + t^8.05 + 2*t^8.14 + t^8.33 + t^8.38 + t^8.48 + t^8.62 + t^8.67 + 2*t^8.71 + t^8.76 + 2*t^8.95 + t^8.71/y^2 - t^3.9/y - t^4.81/y - t^6.33/y - t^6.62/y - t^6.9/y - t^7.19/y - t^7.24/y - t^7.52/y + t^7.81/y + t^8.1/y + t^8.14/y + (2*t^8.38)/y + t^8.67/y + (2*t^8.71)/y - t^8.76/y - t^3.9*y - t^4.81*y - t^6.33*y - t^6.62*y - t^6.9*y - t^7.19*y - t^7.24*y - t^7.52*y + t^7.81*y + t^8.1*y + t^8.14*y + 2*t^8.38*y + t^8.67*y + 2*t^8.71*y - t^8.76*y + t^8.71*y^2 | t^2.38/g1^12 + g1^18*t^2.43 + g1^9*t^2.71 + t^3. + t^3.29/g1^9 + g1^12*t^3.62 + g1^3*t^3.9 + t^4.19/g1^6 + g1^15*t^4.52 + t^4.76/g1^24 + g1^6*t^4.81 + g1^36*t^4.86 + (2*t^5.1)/g1^3 + g1^27*t^5.14 + t^5.38/g1^12 + 2*g1^18*t^5.43 + t^5.67/g1^21 + g1^9*t^5.71 + t^5.95/g1^30 + g1^30*t^6.05 + t^6.24/g1^39 + t^6.29/g1^9 + g1^21*t^6.33 + t^6.57/g1^18 + 2*g1^12*t^6.62 + 2*g1^3*t^6.9 + g1^33*t^6.95 + t^7.14/g1^36 + (2*t^7.19)/g1^6 + 2*g1^24*t^7.24 + g1^54*t^7.29 + (2*t^7.48)/g1^15 + 2*g1^15*t^7.52 + g1^45*t^7.57 + t^7.76/g1^24 + 4*g1^6*t^7.81 + 2*g1^36*t^7.86 + t^8.05/g1^33 + 2*g1^27*t^8.14 + t^8.33/g1^42 + t^8.38/g1^12 + g1^48*t^8.48 + t^8.62/g1^51 + t^8.67/g1^21 + 2*g1^9*t^8.71 + g1^39*t^8.76 + (2*t^8.95)/g1^30 + (g1^9*t^8.71)/y^2 - (g1^3*t^3.9)/y - (g1^6*t^4.81)/y - (g1^21*t^6.33)/y - (g1^12*t^6.62)/y - (g1^3*t^6.9)/y - t^7.19/(g1^6*y) - (g1^24*t^7.24)/y - (g1^15*t^7.52)/y + (g1^6*t^7.81)/y + t^8.1/(g1^3*y) + (g1^27*t^8.14)/y + (2*t^8.38)/(g1^12*y) + t^8.67/(g1^21*y) + (2*g1^9*t^8.71)/y - (g1^39*t^8.76)/y - g1^3*t^3.9*y - g1^6*t^4.81*y - g1^21*t^6.33*y - g1^12*t^6.62*y - g1^3*t^6.9*y - (t^7.19*y)/g1^6 - g1^24*t^7.24*y - g1^15*t^7.52*y + g1^6*t^7.81*y + (t^8.1*y)/g1^3 + g1^27*t^8.14*y + (2*t^8.38*y)/g1^12 + (t^8.67*y)/g1^21 + 2*g1^9*t^8.71*y - g1^39*t^8.76*y + g1^9*t^8.71*y^2 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 57393 | SU3adj1nf2 | ${}M_{1}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ + ${ }q_{2}^{2}\tilde{q}_{2}^{2}$ | 1.4496 | 1.6311 | 0.8887 | [X:[1.3652], M:[0.9043], q:[0.5124, 0.484], qb:[0.5833, 0.516], phi:[0.3174]] | t^2.713 + t^2.856 + t^3. + t^3.085 + t^3.202 + t^3.952 + t^4.038 + t^4.096 + t^4.154 + t^4.239 + t^4.904 + t^4.99 + t^5.106 + t^5.191 + t^5.393 + t^5.426 + t^5.479 + t^5.569 + 2*t^5.713 + t^5.798 + t^5.856 + t^5.942 - 2*t^6. - t^3.952/y - t^4.904/y - t^3.952*y - t^4.904*y | detail |