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 |
|---|---|---|---|---|---|---|---|---|---|
| 57929 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$ | 1.4397 | 1.6242 | 0.8864 | [X:[1.3493], M:[0.9525, 0.9997], q:[0.4581, 0.4574], qb:[0.5423, 0.5901], phi:[0.3254]] | [X:[[0, 6]], M:[[-1, -13], [1, -5]], q:[[-1, 10], [1, 0]], qb:[[0, -5], [0, 13]], phi:[[0, -3]]] | 2 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{1}$, ${ }\phi_{1}^{3}$, ${ }M_{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }X_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}q_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}\phi_{1}^{3}$, ${ }M_{1}M_{2}$, ${ }\phi_{1}^{6}$, ${ }M_{2}\phi_{1}^{3}$, ${ }\phi_{1}^{3}q_{2}\tilde{q}_{1}$ | ${}M_{2}^{2}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }M_{1}q_{1}\tilde{q}_{2}$ | -1 | t^2.86 + t^2.93 + 2*t^3. + t^3.14 + 2*t^3.98 + t^4.05 + 2*t^4.12 + 2*t^4.95 + 2*t^5.09 + 2*t^5.1 + t^5.72 + t^5.79 + 2*t^5.86 + 2*t^5.93 - t^6. + 3*t^6.07 + 2*t^6.14 + t^6.29 + t^6.83 + t^6.9 + 2*t^6.91 + t^6.97 + t^6.98 + t^7.04 + 7*t^7.05 + 5*t^7.12 + t^7.19 + t^7.26 + t^7.27 + 2*t^7.81 + 2*t^7.88 + 4*t^7.95 + 2*t^8.02 + 4*t^8.09 + 6*t^8.1 + 8*t^8.24 + t^8.57 + t^8.64 + 2*t^8.71 + 2*t^8.78 - t^8.86 + 2*t^8.93 + t^8.93/y^2 - t^3.98/y - t^4.95/y - t^6.83/y - t^6.9/y - (2*t^6.98)/y - t^7.12/y - t^7.81/y - t^7.88/y - (2*t^7.95)/y - t^8.1/y + t^8.79/y + (2*t^8.86)/y - t^3.98*y - t^4.95*y - t^6.83*y - t^6.9*y - 2*t^6.98*y - t^7.12*y - t^7.81*y - t^7.88*y - 2*t^7.95*y - t^8.1*y + t^8.79*y + 2*t^8.86*y + t^8.93*y^2 | t^2.86/(g1*g2^13) + t^2.93/g2^9 + (2*g1*t^3.)/g2^5 + (g2^23*t^3.14)/g1 + (g1*t^3.98)/g2^8 + (g2^2*t^3.98)/g1 + g2^6*t^4.05 + g1*g2^10*t^4.12 + (g2^20*t^4.12)/g1 + (g1*t^4.95)/g2^11 + t^4.95/(g1*g2) + 2*g1*g2^7*t^5.09 + (2*g2^17*t^5.1)/g1 + t^5.72/(g1^2*g2^26) + t^5.79/(g1*g2^22) + (2*t^5.86)/g2^18 + (2*g1*t^5.93)/g2^14 - 3*t^6. + (2*g1^2*t^6.)/g2^10 + g1*g2^4*t^6.07 + (2*g2^14*t^6.07)/g1 + 2*g2^18*t^6.14 + (g2^46*t^6.29)/g1^2 + t^6.83/(g1^2*g2^11) + (g1*t^6.9)/g2^17 + (2*t^6.91)/(g1*g2^7) + (g1^2*t^6.97)/g2^13 + t^6.98/g2^3 + (g1^3*t^7.04)/g2^9 + 4*g1*g2*t^7.05 + (2*g2^11*t^7.05)/g1 + (g2^21*t^7.05)/g1^3 + 2*g1^2*g2^5*t^7.12 + 2*g2^15*t^7.12 + (g2^25*t^7.12)/g1^2 + (g2^29*t^7.19)/g1 + g2^33*t^7.26 + (g2^43*t^7.27)/g1^2 + t^7.81/g2^24 + t^7.81/(g1^2*g2^14) + (g1*t^7.88)/g2^20 + t^7.88/(g1*g2^10) + (g1^2*t^7.95)/g2^16 + (2*t^7.95)/g2^6 + (g2^4*t^7.95)/g1^2 + (g1*t^8.02)/g2^2 + (g2^8*t^8.02)/g1 + 4*g1^2*g2^2*t^8.09 + 5*g2^12*t^8.1 + (g2^22*t^8.1)/g1^2 + g1^2*g2^20*t^8.24 + 4*g2^30*t^8.24 + (3*g2^40*t^8.24)/g1^2 + t^8.57/(g1^3*g2^39) + t^8.64/(g1^2*g2^35) + (2*t^8.71)/(g1*g2^31) + (2*t^8.78)/g2^27 + (2*g1*t^8.86)/g2^23 - (3*t^8.86)/(g1*g2^13) + (2*g1^2*t^8.93)/g2^19 - t^8.93/g2^9 + (g2*t^8.93)/g1^2 + t^8.93/(g2^9*y^2) - t^3.98/(g2^3*y) - t^4.95/(g2^6*y) - t^6.83/(g1*g2^16*y) - t^6.9/(g2^12*y) - (2*g1*t^6.98)/(g2^8*y) - (g2^20*t^7.12)/(g1*y) - t^7.81/(g1*g2^19*y) - t^7.88/(g2^15*y) - (2*g1*t^7.95)/(g2^11*y) - (g2^17*t^8.1)/(g1*y) + t^8.79/(g1*g2^22*y) + (2*t^8.86)/(g2^18*y) + (g1*t^8.93)/(g2^14*y) - t^8.93/(g1*g2^4*y) - (t^3.98*y)/g2^3 - (t^4.95*y)/g2^6 - (t^6.83*y)/(g1*g2^16) - (t^6.9*y)/g2^12 - (2*g1*t^6.98*y)/g2^8 - (g2^20*t^7.12*y)/g1 - (t^7.81*y)/(g1*g2^19) - (t^7.88*y)/g2^15 - (2*g1*t^7.95*y)/g2^11 - (g2^17*t^8.1*y)/g1 + (t^8.79*y)/(g1*g2^22) + (2*t^8.86*y)/g2^18 + (g1*t^8.93*y)/g2^14 - (t^8.93*y)/(g1*g2^4) + (t^8.93*y^2)/g2^9 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 57278 | SU3adj1nf2 | ${}q_{1}q_{2}\tilde{q}_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ | 1.4543 | 1.6397 | 0.8869 | [X:[1.3446], M:[0.9663, 0.9998], q:[0.5085, 0.5081], qb:[0.4917, 0.5255], phi:[0.3277]] | t^2.899 + t^2.949 + 2*t^2.999 + t^3.102 + t^3.982 + t^3.984 + t^4.034 + t^4.084 + t^4.085 + t^4.966 + t^4.967 + t^5.067 + t^5.068 + t^5.51 + t^5.557 + t^5.559 + t^5.611 + t^5.798 + t^5.848 + 2*t^5.898 + 2*t^5.949 + 2*t^5.999 - 4*t^6. - t^3.983/y - t^4.966/y - t^3.983*y - t^4.966*y | detail |