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 |
|---|---|---|---|---|---|---|---|---|---|
| 59417 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }q_{1}\tilde{q}_{2}X_{1}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ | 1.1412 | 1.3478 | 0.8467 | [X:[1.5919], M:[1.1837], q:[0.1768, 0.4628], qb:[0.6802, 0.2314], phi:[0.4081]] | [X:[[3]], M:[[6]], q:[[-16], [26]], qb:[[-5], [13]], phi:[[-3]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{1}$, ${ }\phi_{1}^{3}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }X_{1}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}^{2}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{1}^{3}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}\tilde{q}_{2}^{3}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$ | ${}$ | -2 | t^2.08 + t^2.45 + t^2.57 + t^3.31 + t^3.43 + t^3.55 + 3*t^3.67 + t^3.8 + t^4.16 + 3*t^4.53 + 2*t^4.65 + t^4.78 + 2*t^4.9 + 2*t^5.02 + t^5.26 + t^5.39 + t^5.51 + t^5.63 + 6*t^5.76 + 3*t^5.88 - 2*t^6. + 5*t^6.12 + 3*t^6.24 + t^6.25 + 4*t^6.61 + 3*t^6.74 + t^6.86 + 8*t^6.98 + 7*t^7.1 + 7*t^7.35 + 6*t^7.47 + t^7.71 + t^7.72 + 10*t^7.84 + 5*t^7.96 - 3*t^8.08 + 12*t^8.2 + 11*t^8.33 - 3*t^8.45 + 3*t^8.57 + 7*t^8.69 + 4*t^8.7 + 2*t^8.82 + 3*t^8.94 - t^4.22/y - t^5.45/y - t^6.31/y - t^6.8/y - (2*t^7.9)/y + t^8.51/y + t^8.63/y + (3*t^8.76)/y + (3*t^8.88)/y - t^4.22*y - t^5.45*y - t^6.31*y - t^6.8*y - 2*t^7.9*y + t^8.51*y + t^8.63*y + 3*t^8.76*y + 3*t^8.88*y | g1^39*t^2.08 + t^2.45/g1^6 + t^2.57/g1^21 + g1^36*t^3.31 + g1^21*t^3.43 + g1^6*t^3.55 + (3*t^3.67)/g1^9 + t^3.8/g1^24 + g1^78*t^4.16 + 3*g1^33*t^4.53 + 2*g1^18*t^4.65 + g1^3*t^4.78 + (2*t^4.9)/g1^12 + (2*t^5.02)/g1^27 + t^5.26/g1^57 + g1^75*t^5.39 + g1^60*t^5.51 + g1^45*t^5.63 + 6*g1^30*t^5.76 + 3*g1^15*t^5.88 - 2*t^6. + (5*t^6.12)/g1^15 + (3*t^6.24)/g1^30 + g1^117*t^6.25 + 4*g1^72*t^6.61 + 3*g1^57*t^6.74 + g1^42*t^6.86 + 8*g1^27*t^6.98 + 7*g1^12*t^7.1 + (7*t^7.35)/g1^18 + (5*t^7.47)/g1^33 + g1^114*t^7.47 - t^7.59/g1^48 + g1^99*t^7.59 + t^7.71/g1^63 + g1^84*t^7.72 + t^7.84/g1^78 + 9*g1^69*t^7.84 + 5*g1^54*t^7.96 - 3*g1^39*t^8.08 + 12*g1^24*t^8.2 + 10*g1^9*t^8.33 + g1^156*t^8.33 - (3*t^8.45)/g1^6 + (3*t^8.57)/g1^21 + (7*t^8.69)/g1^36 + 4*g1^111*t^8.7 - t^8.82/g1^51 + 3*g1^96*t^8.82 + (2*t^8.94)/g1^66 + g1^81*t^8.94 - t^4.22/(g1^3*y) - t^5.45/(g1^6*y) - (g1^36*t^6.31)/y - t^6.8/(g1^24*y) - (2*t^7.9)/(g1^12*y) + (g1^60*t^8.51)/y + (g1^45*t^8.63)/y + (3*g1^30*t^8.76)/y + (3*g1^15*t^8.88)/y - (t^4.22*y)/g1^3 - (t^5.45*y)/g1^6 - g1^36*t^6.31*y - (t^6.8*y)/g1^24 - (2*t^7.9*y)/g1^12 + g1^60*t^8.51*y + g1^45*t^8.63*y + 3*g1^30*t^8.76*y + 3*g1^15*t^8.88*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 |
|---|---|---|---|---|---|---|---|---|---|
| 57728 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }q_{1}\tilde{q}_{2}X_{1}$ | 1.1613 | 1.3662 | 0.85 | [X:[1.594], M:[1.1879], q:[0.2239, 0.5394], qb:[0.6183, 0.1822], phi:[0.406]] | t^2.16 + t^2.44 + t^2.53 + t^3.38 + t^3.47 + t^3.56 + 2*t^3.65 + t^3.74 + t^4.17 + t^4.18 + t^4.33 + 2*t^4.6 + t^4.69 + t^4.78 + t^4.87 + 2*t^4.96 + t^5.13 + t^5.29 + t^5.38 + t^5.4 + t^5.47 + t^5.55 + t^5.64 + t^5.67 + t^5.73 + 3*t^5.82 + 3*t^5.91 - 3*t^6. - t^4.22/y - t^5.44/y - t^4.22*y - t^5.44*y | detail |