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 |
|---|---|---|---|---|---|---|---|---|---|
| 1161 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{1}M_{5}$ + ${ }M_{6}q_{1}q_{2}$ | 0.6614 | 0.8199 | 0.8067 | [M:[1.1633, 1.085, 0.9541, 0.8367, 0.8367, 0.8759], q:[0.7713, 0.3529], qb:[0.4838, 0.5621], phi:[0.4575]] | [M:[[8], [-4], [10], [-8], [-8], [-2]], q:[[-1], [3]], qb:[[-11], [1]], phi:[[2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }M_{5}$, ${ }M_{6}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{3}M_{5}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{3}M_{6}$, ${ }\phi_{1}^{4}$, ${ }M_{3}^{2}$, ${ }M_{2}M_{4}$, ${ }M_{2}M_{5}$, ${ }M_{2}M_{6}$ | ${}$ | -2 | 2*t^2.51 + t^2.628 + t^2.745 + t^2.862 + t^3.255 + t^3.765 + t^3.883 + t^4. + t^4.117 + t^4.276 + t^4.51 + t^4.745 + 3*t^5.02 + 2*t^5.138 + 3*t^5.255 + 2*t^5.372 + 2*t^5.49 + t^5.724 + t^5.765 + t^5.883 - 2*t^6. - t^6.235 + 2*t^6.276 + 2*t^6.393 + 3*t^6.51 + 2*t^6.628 + 2*t^6.786 + t^6.862 + t^6.903 + 3*t^7.02 + t^7.138 + t^7.255 + 5*t^7.531 + 3*t^7.648 + 5*t^7.765 + 4*t^7.883 + 3*t^8. + t^8.041 + t^8.117 + t^8.158 + 2*t^8.235 + 2*t^8.276 + t^8.352 + t^8.393 - 3*t^8.51 + t^8.551 + t^8.587 - 3*t^8.628 - 3*t^8.745 + 4*t^8.786 - 3*t^8.862 + 3*t^8.903 - t^8.98 - t^4.372/y - t^6.883/y - t^7./y - t^7.235/y + t^7.51/y + t^7.745/y + t^7.862/y + t^8.02/y + (2*t^8.138)/y + (2*t^8.255)/y + (3*t^8.372)/y + t^8.49/y + t^8.607/y + (2*t^8.765)/y + t^8.883/y - t^4.372*y - t^6.883*y - t^7.*y - t^7.235*y + t^7.51*y + t^7.745*y + t^7.862*y + t^8.02*y + 2*t^8.138*y + 2*t^8.255*y + 3*t^8.372*y + t^8.49*y + t^8.607*y + 2*t^8.765*y + t^8.883*y | (2*t^2.51)/g1^8 + t^2.628/g1^2 + g1^4*t^2.745 + g1^10*t^2.862 + t^3.255/g1^4 + t^3.765/g1^12 + t^3.883/g1^6 + t^4. + g1^6*t^4.117 + t^4.276/g1^20 + t^4.51/g1^8 + g1^4*t^4.745 + (3*t^5.02)/g1^16 + (2*t^5.138)/g1^10 + (3*t^5.255)/g1^4 + 2*g1^2*t^5.372 + 2*g1^8*t^5.49 + g1^20*t^5.724 + t^5.765/g1^12 + t^5.883/g1^6 - 2*t^6. - g1^12*t^6.235 + (2*t^6.276)/g1^20 + (2*t^6.393)/g1^14 + (3*t^6.51)/g1^8 + (2*t^6.628)/g1^2 + (2*t^6.786)/g1^28 + g1^10*t^6.862 + t^6.903/g1^22 + (3*t^7.02)/g1^16 + t^7.138/g1^10 + t^7.255/g1^4 + (5*t^7.531)/g1^24 + (3*t^7.648)/g1^18 + (5*t^7.765)/g1^12 + (4*t^7.883)/g1^6 + 3*t^8. + t^8.041/g1^32 + g1^6*t^8.117 + t^8.158/g1^26 + 2*g1^12*t^8.235 + (2*t^8.276)/g1^20 + g1^18*t^8.352 + t^8.393/g1^14 - (3*t^8.51)/g1^8 + t^8.551/g1^40 + g1^30*t^8.587 - (3*t^8.628)/g1^2 - 3*g1^4*t^8.745 + (4*t^8.786)/g1^28 - 3*g1^10*t^8.862 + (3*t^8.903)/g1^22 - g1^16*t^8.98 - (g1^2*t^4.372)/y - t^6.883/(g1^6*y) - t^7./y - (g1^12*t^7.235)/y + t^7.51/(g1^8*y) + (g1^4*t^7.745)/y + (g1^10*t^7.862)/y + t^8.02/(g1^16*y) + (2*t^8.138)/(g1^10*y) + (2*t^8.255)/(g1^4*y) + (3*g1^2*t^8.372)/y + (g1^8*t^8.49)/y + (g1^14*t^8.607)/y + (2*t^8.765)/(g1^12*y) + t^8.883/(g1^6*y) - g1^2*t^4.372*y - (t^6.883*y)/g1^6 - t^7.*y - g1^12*t^7.235*y + (t^7.51*y)/g1^8 + g1^4*t^7.745*y + g1^10*t^7.862*y + (t^8.02*y)/g1^16 + (2*t^8.138*y)/g1^10 + (2*t^8.255*y)/g1^4 + 3*g1^2*t^8.372*y + g1^8*t^8.49*y + g1^14*t^8.607*y + (2*t^8.765*y)/g1^12 + (t^8.883*y)/g1^6 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 711 | SU2adj1nf2 | ${}\phi_{1}q_{1}^{2}$ + ${ }M_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}q_{2}\tilde{q}_{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{4}$ + ${ }M_{1}M_{5}$ | 0.6503 | 0.8006 | 0.8123 | [M:[1.1584, 1.0875, 0.948, 0.8416, 0.8416], q:[0.7719, 0.3511], qb:[0.4905, 0.5615], phi:[0.4563]] | 2*t^2.525 + t^2.738 + t^2.844 + t^3.262 + t^3.369 + t^3.787 + t^3.894 + t^4. + t^4.106 + t^4.312 + t^4.525 + t^4.738 + 3*t^5.05 + 2*t^5.262 + t^5.369 + t^5.475 + t^5.688 + t^5.787 + 2*t^5.894 - 2*t^6. - t^4.369/y - t^4.369*y | detail |