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 |
|---|---|---|---|---|---|---|---|---|---|
| 59020 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{1}\phi_{1}^{3}$ | 1.3874 | 1.6013 | 0.8664 | [X:[1.277], M:[0.9155], q:[0.6182, 0.4022], qb:[0.4898, 0.3208], phi:[0.3615]] | [X:[[6]], M:[[9]], q:[[17], [-31]], qb:[[7], [25]], phi:[[-3]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}q_{2}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{3}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ | ${}q_{2}\tilde{q}_{2}X_{1}$ | 0 | t^2.17 + t^2.68 + t^2.75 + t^2.82 + t^3.25 + t^3.32 + t^3.76 + t^3.83 + t^3.9 + 2*t^4.34 + t^4.41 + t^4.48 + 2*t^4.85 + t^4.92 + 3*t^4.99 + t^5.35 + 2*t^5.42 + 3*t^5.49 + 2*t^5.56 + t^5.63 + 2*t^5.93 + 4*t^6.07 + 2*t^6.14 + t^6.44 + 4*t^6.51 + 3*t^6.58 + 4*t^6.65 + t^6.72 + t^6.87 + 4*t^7.01 + 2*t^7.08 + 8*t^7.15 + 2*t^7.23 + t^7.3 + 3*t^7.52 + 2*t^7.59 + 7*t^7.66 + 5*t^7.73 + 4*t^7.8 + 4*t^8.1 + 2*t^8.17 + 9*t^8.24 + 6*t^8.31 + 3*t^8.38 + t^8.45 - t^8.54 + 3*t^8.61 + 2*t^8.68 + 5*t^8.75 + 7*t^8.82 + 6*t^8.89 + 3*t^8.96 - t^4.08/y - t^5.17/y - t^6.25/y - t^6.76/y - t^6.83/y - t^6.9/y - t^7.34/y - t^7.41/y + t^8.49/y + t^8.56/y - t^4.08*y - t^5.17*y - t^6.25*y - t^6.76*y - t^6.83*y - t^6.9*y - t^7.34*y - t^7.41*y + t^8.49*y + t^8.56*y | t^2.17/g1^6 + t^2.68/g1^24 + g1^9*t^2.75 + g1^42*t^2.82 + t^3.25/g1^9 + g1^24*t^3.32 + t^3.76/g1^27 + g1^6*t^3.83 + g1^39*t^3.9 + (2*t^4.34)/g1^12 + g1^21*t^4.41 + g1^54*t^4.48 + (2*t^4.85)/g1^30 + g1^3*t^4.92 + 3*g1^36*t^4.99 + t^5.35/g1^48 + (2*t^5.42)/g1^15 + 3*g1^18*t^5.49 + 2*g1^51*t^5.56 + g1^84*t^5.63 + (2*t^5.93)/g1^33 + 4*g1^33*t^6.07 + 2*g1^66*t^6.14 + t^6.44/g1^51 + (4*t^6.51)/g1^18 + 3*g1^15*t^6.58 + 4*g1^48*t^6.65 + g1^81*t^6.72 + t^6.87/g1^102 + (4*t^7.01)/g1^36 + (2*t^7.08)/g1^3 + 8*g1^30*t^7.15 + 2*g1^63*t^7.23 + g1^96*t^7.3 + (3*t^7.52)/g1^54 + (2*t^7.59)/g1^21 + 7*g1^12*t^7.66 + 5*g1^45*t^7.73 + 4*g1^78*t^7.8 + (4*t^8.1)/g1^39 + (2*t^8.17)/g1^6 + 9*g1^27*t^8.24 + 6*g1^60*t^8.31 + 3*g1^93*t^8.38 + g1^126*t^8.45 - t^8.54/g1^90 + (3*t^8.61)/g1^57 + (2*t^8.68)/g1^24 + 5*g1^9*t^8.75 + 7*g1^42*t^8.82 + 6*g1^75*t^8.89 + 3*g1^108*t^8.96 - t^4.08/(g1^3*y) - t^5.17/(g1^6*y) - t^6.25/(g1^9*y) - t^6.76/(g1^27*y) - (g1^6*t^6.83)/y - (g1^39*t^6.9)/y - t^7.34/(g1^12*y) - (g1^21*t^7.41)/y + (g1^18*t^8.49)/y + (g1^51*t^8.56)/y - (t^4.08*y)/g1^3 - (t^5.17*y)/g1^6 - (t^6.25*y)/g1^9 - (t^6.76*y)/g1^27 - g1^6*t^6.83*y - g1^39*t^6.9*y - (t^7.34*y)/g1^12 - g1^21*t^7.41*y + g1^18*t^8.49*y + g1^51*t^8.56*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 |
|---|---|---|---|---|---|---|---|---|---|
| 57694 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }\phi_{1}q_{1}^{2}q_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}q_{2}\tilde{q}_{2}$ | 1.4624 | 1.6668 | 0.8773 | [X:[1.3429], M:[0.6714], q:[0.5762, 0.519], qb:[0.4524, 0.481], phi:[0.3286]] | t^2.01 + t^2.91 + t^2.96 + t^3. + t^3.09 + t^3.17 + t^3.9 + 2*t^4.03 + t^4.07 + t^4.16 + t^4.89 + t^4.93 + 2*t^4.97 + t^5.01 + t^5.06 + t^5.1 + 2*t^5.14 + t^5.19 + t^5.23 + t^5.83 + t^5.87 + 2*t^5.91 + t^5.96 - t^6. - t^3.99/y - t^4.97/y - t^6./y - t^3.99*y - t^4.97*y - t^6.*y | detail |