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 |
|---|---|---|---|---|---|---|---|---|---|
| 5457 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{3}M_{5}$ + ${ }\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{4}X_{1}$ + ${ }M_{6}\phi_{1}q_{1}^{2}$ + ${ }M_{7}q_{1}\tilde{q}_{2}$ + ${ }M_{6}M_{7}$ + ${ }M_{7}M_{8}$ | 0.603 | 0.7529 | 0.801 | [X:[1.6007], M:[0.8022, 0.795, 1.1978, 0.3993, 0.8022, 1.0018, 0.9982, 1.0018], q:[0.2995, 0.8984], qb:[0.5027, 0.7023], phi:[0.3993]] | [X:[[4]], M:[[12], [-28], [-12], [-4], [12], [10], [-10], [10]], q:[[-3], [-9]], qb:[[15], [13]], phi:[[-4]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }M_{5}$, ${ }M_{6}$, ${ }M_{8}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{2}^{2}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{1}M_{2}$, ${ }M_{2}M_{5}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }X_{1}$, ${ }M_{1}^{2}$, ${ }M_{1}M_{5}$, ${ }M_{5}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{2}M_{6}$, ${ }M_{2}M_{8}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{8}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{1}M_{8}$, ${ }M_{5}M_{8}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$ | ${}\phi_{1}^{3}q_{1}\tilde{q}_{1}$ | -2 | t^2.385 + t^2.396 + 2*t^2.406 + 2*t^3.005 + t^3.604 + t^4.203 + t^4.214 + t^4.77 + t^4.781 + 3*t^4.791 + 3*t^4.802 + 3*t^4.813 + t^5.39 + t^5.401 + 4*t^5.412 - 2*t^6. + 4*t^6.011 - t^6.599 + 3*t^6.61 + 2*t^6.62 + t^7.155 + t^7.166 + 3*t^7.176 + 3*t^7.187 + 3*t^7.198 + 4*t^7.209 + 5*t^7.219 + t^7.775 + t^7.797 + 2*t^7.808 + 6*t^7.818 - 3*t^8.385 - 2*t^8.396 - 4*t^8.406 + 7*t^8.417 + t^8.428 - t^8.984 - t^8.995 - t^4.198/y - t^6.583/y - t^6.594/y - t^6.604/y + t^7.192/y - t^7.203/y + t^7.781/y + (3*t^7.791)/y + (3*t^7.802)/y + (2*t^7.813)/y + (2*t^8.39)/y + (2*t^8.401)/y + (4*t^8.412)/y - t^8.968/y - t^8.978/y - t^8.989/y - t^4.198*y - t^6.583*y - t^6.594*y - t^6.604*y + t^7.192*y - t^7.203*y + t^7.781*y + 3*t^7.791*y + 3*t^7.802*y + 2*t^7.813*y + 2*t^8.39*y + 2*t^8.401*y + 4*t^8.412*y - t^8.968*y - t^8.978*y - t^8.989*y | t^2.385/g1^28 + t^2.396/g1^8 + 2*g1^12*t^2.406 + 2*g1^10*t^3.005 + g1^8*t^3.604 + g1^6*t^4.203 + g1^26*t^4.214 + t^4.77/g1^56 + t^4.781/g1^36 + (3*t^4.791)/g1^16 + 3*g1^4*t^4.802 + 3*g1^24*t^4.813 + t^5.39/g1^18 + g1^2*t^5.401 + 4*g1^22*t^5.412 - 2*t^6. + 4*g1^20*t^6.011 - t^6.599/g1^2 + 3*g1^18*t^6.61 + 2*g1^38*t^6.62 + t^7.155/g1^84 + t^7.166/g1^64 + (3*t^7.176)/g1^44 + (3*t^7.187)/g1^24 + (3*t^7.198)/g1^4 + 4*g1^16*t^7.209 + 5*g1^36*t^7.219 + t^7.775/g1^46 + t^7.797/g1^6 + 2*g1^14*t^7.808 + 6*g1^34*t^7.818 - (3*t^8.385)/g1^28 - (2*t^8.396)/g1^8 - 4*g1^12*t^8.406 + 7*g1^32*t^8.417 + g1^52*t^8.428 - t^8.984/g1^30 - t^8.995/g1^10 - t^4.198/(g1^4*y) - t^6.583/(g1^32*y) - t^6.594/(g1^12*y) - (g1^8*t^6.604)/y + t^7.192/(g1^14*y) - (g1^6*t^7.203)/y + t^7.781/(g1^36*y) + (3*t^7.791)/(g1^16*y) + (3*g1^4*t^7.802)/y + (2*g1^24*t^7.813)/y + (2*t^8.39)/(g1^18*y) + (2*g1^2*t^8.401)/y + (4*g1^22*t^8.412)/y - t^8.968/(g1^60*y) - t^8.978/(g1^40*y) - t^8.989/(g1^20*y) - (t^4.198*y)/g1^4 - (t^6.583*y)/g1^32 - (t^6.594*y)/g1^12 - g1^8*t^6.604*y + (t^7.192*y)/g1^14 - g1^6*t^7.203*y + (t^7.781*y)/g1^36 + (3*t^7.791*y)/g1^16 + 3*g1^4*t^7.802*y + 2*g1^24*t^7.813*y + (2*t^8.39*y)/g1^18 + 2*g1^2*t^8.401*y + 4*g1^22*t^8.412*y - (t^8.968*y)/g1^60 - (t^8.978*y)/g1^40 - (t^8.989*y)/g1^20 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 3853 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{3}M_{5}$ + ${ }\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{4}X_{1}$ + ${ }M_{6}\phi_{1}q_{1}^{2}$ + ${ }M_{7}q_{1}\tilde{q}_{2}$ + ${ }M_{6}M_{7}$ | 0.6036 | 0.7534 | 0.8013 | [X:[1.6046], M:[0.8137, 0.768, 1.1863, 0.3954, 0.8137, 1.0114, 0.9886], q:[0.2966, 0.8897], qb:[0.5171, 0.7149], phi:[0.3954]] | t^2.304 + t^2.373 + 2*t^2.441 + t^2.966 + t^3.034 + t^3.627 + t^4.221 + t^4.289 + t^4.608 + t^4.677 + 3*t^4.745 + 3*t^4.814 + 3*t^4.882 + t^5.27 + t^5.338 + 2*t^5.407 + 2*t^5.475 + t^5.931 - t^6. - t^4.186/y - t^4.186*y | detail |