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 |
|---|---|---|---|---|---|---|---|---|---|
| 58102 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}^{3}$ + ${ }\phi_{1}q_{1}q_{2}^{2}$ | 1.4376 | 1.6261 | 0.8841 | [X:[1.3313], M:[0.9969], q:[0.5511, 0.5573], qb:[0.4489, 0.4366], phi:[0.3344]] | [X:[[6]], M:[[9]], q:[[13], [-5]], qb:[[-13], [23]], phi:[[-3]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}q_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{1}$, ${ }q_{1}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }X_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}\tilde{q}_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}^{2}$, ${ }\phi_{1}q_{1}^{2}q_{2}$, ${ }q_{1}q_{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{1}q_{1}\tilde{q}_{1}$ | ${}$ | -1 | t^2.96 + t^2.98 + t^2.99 + t^3. + t^3.02 + t^3.97 + t^3.98 + t^3.99 + t^4. + t^4.02 + 2*t^4.97 + t^4.99 + 2*t^5.01 + t^5.02 + t^5.93 + t^5.94 + t^5.95 + t^5.96 + 2*t^5.97 + 3*t^5.98 + t^5.99 - t^6. + 2*t^6.01 + t^6.93 + t^6.94 + 2*t^6.95 + 2*t^6.96 + 2*t^6.97 + 7*t^6.98 + 2*t^6.99 + 3*t^7.01 + t^7.02 + t^7.05 + 3*t^7.93 + 3*t^7.95 + 2*t^7.96 + 6*t^7.97 + 6*t^7.99 + 2*t^8. + 3*t^8.01 + 3*t^8.02 + t^8.89 + t^8.91 + t^8.92 + t^8.93 + 7*t^8.94 + 4*t^8.95 + 8*t^8.97 - 2*t^8.98 + 3*t^8.99 - t^4./y - t^5.01/y - t^6.97/y - t^6.98/y - t^6.99/y - t^7./y - t^7.02/y - t^7.97/y - t^7.99/y - t^8./y - t^8.01/y - t^8.02/y + t^8.94/y + t^8.95/y + t^8.96/y + (2*t^8.98)/y - t^4.*y - t^5.01*y - t^6.97*y - t^6.98*y - t^6.99*y - t^7.*y - t^7.02*y - t^7.97*y - t^7.99*y - t^8.*y - t^8.01*y - t^8.02*y + t^8.94*y + t^8.95*y + t^8.96*y + 2*t^8.98*y | g1^36*t^2.96 + g1^18*t^2.98 + g1^9*t^2.99 + t^3. + t^3.02/g1^18 + g1^33*t^3.97 + g1^15*t^3.98 + g1^6*t^3.99 + t^4./g1^3 + t^4.02/g1^21 + 2*g1^30*t^4.97 + g1^12*t^4.99 + (2*t^5.01)/g1^6 + t^5.02/g1^24 + g1^72*t^5.93 + g1^54*t^5.94 + g1^45*t^5.95 + g1^36*t^5.96 + 2*g1^27*t^5.97 + 3*g1^18*t^5.98 + g1^9*t^5.99 - t^6. + (2*t^6.01)/g1^9 + g1^69*t^6.93 + g1^60*t^6.94 + 2*g1^51*t^6.95 + 2*g1^42*t^6.96 + 2*g1^33*t^6.97 + 4*g1^15*t^6.98 + 3*g1^24*t^6.98 + 2*g1^6*t^6.99 + (3*t^7.01)/g1^12 + t^7.02/g1^21 + t^7.05/g1^48 + 3*g1^66*t^7.93 + 3*g1^48*t^7.95 + 2*g1^39*t^7.96 + 6*g1^30*t^7.97 + 6*g1^12*t^7.99 + 2*g1^3*t^8. + (3*t^8.01)/g1^6 + (3*t^8.02)/g1^24 + g1^108*t^8.89 + g1^90*t^8.91 + g1^81*t^8.92 + g1^72*t^8.93 + 3*g1^54*t^8.94 + 4*g1^63*t^8.94 + 4*g1^45*t^8.95 + 8*g1^27*t^8.97 - 2*g1^18*t^8.98 + 3*g1^9*t^8.99 - t^4./(g1^3*y) - t^5.01/(g1^6*y) - (g1^33*t^6.97)/y - (g1^15*t^6.98)/y - (g1^6*t^6.99)/y - t^7./(g1^3*y) - t^7.02/(g1^21*y) - (g1^30*t^7.97)/y - (g1^12*t^7.99)/y - (g1^3*t^8.)/y - t^8.01/(g1^6*y) - t^8.02/(g1^24*y) + (g1^54*t^8.94)/y + (g1^45*t^8.95)/y + (g1^36*t^8.96)/y + (2*g1^18*t^8.98)/y - (t^4.*y)/g1^3 - (t^5.01*y)/g1^6 - g1^33*t^6.97*y - g1^15*t^6.98*y - g1^6*t^6.99*y - (t^7.*y)/g1^3 - (t^7.02*y)/g1^21 - g1^30*t^7.97*y - g1^12*t^7.99*y - g1^3*t^8.*y - (t^8.01*y)/g1^6 - (t^8.02*y)/g1^24 + g1^54*t^8.94*y + g1^45*t^8.95*y + g1^36*t^8.96*y + 2*g1^18*t^8.98*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 |
|---|---|---|---|---|---|---|---|---|---|
| 57334 | SU3adj1nf2 | ${}q_{1}^{2}\tilde{q}_{1}^{2}$ + ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}^{2}X_{1}$ + ${ }M_{1}\phi_{1}^{3}$ | 1.4535 | 1.6425 | 0.8849 | [X:[1.3301], M:[0.9951], q:[0.4926, 0.5024], qb:[0.5074, 0.4878], phi:[0.335]] | t^2.941 + t^2.971 + t^2.985 + t^3. + t^3.029 + t^3.946 + t^3.976 + t^3.99 + t^4.005 + t^4.034 + t^4.951 + t^4.98 + t^5.01 + t^5.039 + t^5.454 + t^5.468 + t^5.497 + t^5.513 + t^5.883 + t^5.912 + t^5.927 + t^5.941 + t^5.956 + 2*t^5.971 + t^5.985 - 2*t^6. - t^4.005/y - t^5.01/y - t^4.005*y - t^5.01*y | detail |