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 |
|---|---|---|---|---|---|---|---|---|---|
| 57109 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ + ${ }M_{3}M_{5}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}M_{6}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{6}M_{7}$ | 0.7132 | 0.8851 | 0.8057 | [M:[0.6737, 0.7253, 1.0258, 0.9742, 0.9742, 1.2747, 0.7253], q:[0.7876, 0.5387], qb:[0.4871, 0.4871], phi:[0.4249]] | [M:[[22], [-6], [-14], [14], [14], [6], [-6]], q:[[-1], [-21]], qb:[[7], [7]], phi:[[2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{1}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{4}$, ${ }M_{5}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{7}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{7}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{1}M_{4}$, ${ }M_{1}M_{5}$, ${ }M_{4}M_{7}$, ${ }M_{5}M_{7}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{7}q_{2}\tilde{q}_{1}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}^{2}$ | ${}M_{4}q_{2}\tilde{q}_{1}$, ${ }M_{7}q_{1}\tilde{q}_{2}$ | -2 | t^2.021 + t^2.176 + t^2.549 + 2*t^2.923 + t^3.077 + t^3.824 + t^4.042 + 4*t^4.197 + 3*t^4.352 + t^4.507 + t^4.57 + t^4.725 + 2*t^4.944 + 4*t^5.099 + t^5.253 + 2*t^5.472 + t^5.627 + 2*t^5.845 - 2*t^6. + t^6.064 - t^6.155 + 4*t^6.218 + 5*t^6.373 + 3*t^6.528 + t^6.592 + t^6.683 + 5*t^6.747 + t^6.901 + 2*t^6.965 + t^7.056 + 8*t^7.12 + 5*t^7.275 + 2*t^7.43 + 2*t^7.493 + t^7.584 + 2*t^7.648 - t^7.803 + 2*t^7.866 - t^7.958 + 2*t^8.021 + t^8.085 - 4*t^8.176 + 4*t^8.24 - 2*t^8.331 + 11*t^8.394 + 4*t^8.549 + t^8.613 + 4*t^8.704 + 6*t^8.768 + 3*t^8.859 - 3*t^8.923 + 2*t^8.986 - t^4.275/y - t^6.296/y - t^6.451/y - t^6.824/y + t^7.352/y + t^7.57/y + (2*t^7.725)/y + (2*t^7.944)/y + (4*t^8.099)/y + (2*t^8.253)/y - t^8.317/y + t^8.472/y + t^8.845/y - t^4.275*y - t^6.296*y - t^6.451*y - t^6.824*y + t^7.352*y + t^7.57*y + 2*t^7.725*y + 2*t^7.944*y + 4*t^8.099*y + 2*t^8.253*y - t^8.317*y + t^8.472*y + t^8.845*y | g1^22*t^2.021 + t^2.176/g1^6 + g1^4*t^2.549 + 2*g1^14*t^2.923 + t^3.077/g1^14 + g1^6*t^3.824 + g1^44*t^4.042 + 4*g1^16*t^4.197 + (3*t^4.352)/g1^12 + t^4.507/g1^40 + g1^26*t^4.57 + t^4.725/g1^2 + 2*g1^36*t^4.944 + 4*g1^8*t^5.099 + t^5.253/g1^20 + 2*g1^18*t^5.472 + t^5.627/g1^10 + 2*g1^28*t^5.845 - 2*t^6. + g1^66*t^6.064 - t^6.155/g1^28 + 4*g1^38*t^6.218 + 5*g1^10*t^6.373 + (3*t^6.528)/g1^18 + g1^48*t^6.592 + t^6.683/g1^46 + 5*g1^20*t^6.747 + t^6.901/g1^8 + 2*g1^58*t^6.965 + t^7.056/g1^36 + 8*g1^30*t^7.12 + 5*g1^2*t^7.275 + (2*t^7.43)/g1^26 + 2*g1^40*t^7.493 + t^7.584/g1^54 + 2*g1^12*t^7.648 - t^7.803/g1^16 + 2*g1^50*t^7.866 - t^7.958/g1^44 + 2*g1^22*t^8.021 + g1^88*t^8.085 - (4*t^8.176)/g1^6 + 4*g1^60*t^8.24 - (2*t^8.331)/g1^34 + 11*g1^32*t^8.394 + 4*g1^4*t^8.549 + g1^70*t^8.613 + (4*t^8.704)/g1^24 + 6*g1^42*t^8.768 + (3*t^8.859)/g1^52 - 3*g1^14*t^8.923 + 2*g1^80*t^8.986 - (g1^2*t^4.275)/y - (g1^24*t^6.296)/y - t^6.451/(g1^4*y) - (g1^6*t^6.824)/y + t^7.352/(g1^12*y) + (g1^26*t^7.57)/y + (2*t^7.725)/(g1^2*y) + (2*g1^36*t^7.944)/y + (4*g1^8*t^8.099)/y + (2*t^8.253)/(g1^20*y) - (g1^46*t^8.317)/y + (g1^18*t^8.472)/y + (g1^28*t^8.845)/y - g1^2*t^4.275*y - g1^24*t^6.296*y - (t^6.451*y)/g1^4 - g1^6*t^6.824*y + (t^7.352*y)/g1^12 + g1^26*t^7.57*y + (2*t^7.725*y)/g1^2 + 2*g1^36*t^7.944*y + 4*g1^8*t^8.099*y + (2*t^8.253*y)/g1^20 - g1^46*t^8.317*y + g1^18*t^8.472*y + g1^28*t^8.845*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 |
|---|---|---|---|---|---|---|---|---|---|
| 55522 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{3}M_{4}$ + ${ }M_{3}M_{5}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{2}M_{6}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ | 0.6933 | 0.8483 | 0.8172 | [M:[0.6702, 0.7263, 1.028, 0.972, 0.972, 1.2737], q:[0.7877, 0.542], qb:[0.486, 0.486], phi:[0.4246]] | t^2.011 + t^2.547 + 2*t^2.916 + t^3.084 + 2*t^3.821 + t^4.021 + 3*t^4.19 + 2*t^4.358 + t^4.526 + t^4.558 + 2*t^4.927 + 2*t^5.095 + 2*t^5.463 + t^5.631 + 3*t^5.832 - 3*t^6. - t^4.274/y - t^4.274*y | detail |