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 |
|---|---|---|---|---|---|---|---|---|---|
| 4791 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}M_{5}$ + ${ }M_{4}M_{7}$ + ${ }M_{1}M_{8}$ | 0.6625 | 0.8215 | 0.8064 | [M:[0.9984, 0.818, 0.9984, 0.818, 1.182, 0.7278, 1.182, 1.0016], q:[0.5925, 0.409], qb:[0.409, 0.7729], phi:[0.4541]] | [M:[[-22], [-2], [-22], [-2], [2], [8], [2], [22]], q:[[23], [-1]], qb:[[-1], [3]], phi:[[-6]]] | 1 | {a: 5744057/8670000, c: 7122757/8670000, M1: 1273/1275, M2: 1043/1275, M3: 1273/1275, M4: 1043/1275, M5: 1507/1275, M6: 928/1275, M7: 1507/1275, M8: 1277/1275, q1: 1511/2550, q2: 1043/2550, qb1: 1043/2550, qb2: 657/850, phi1: 193/425} |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{6}$, ${ }M_{2}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{8}$, ${ }M_{5}$, ${ }M_{7}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{2}M_{6}$, ${ }M_{2}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{2}\phi_{1}^{2}$, ${ }M_{6}M_{8}$, ${ }M_{2}M_{8}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{5}M_{6}$, ${ }M_{6}M_{7}$, ${ }M_{8}\phi_{1}^{2}$, ${ }M_{3}^{2}$ | ${}M_{2}M_{7}$, ${ }M_{3}M_{8}$, ${ }M_{6}\phi_{1}q_{2}^{2}$, ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$ | 0 | t^2.184 + t^2.454 + t^2.725 + t^2.995 + t^3.005 + 2*t^3.546 + 2*t^3.816 + t^4.096 + 3*t^4.367 + t^4.638 + 2*t^4.908 + t^4.918 + 2*t^5.179 + t^5.188 + t^5.459 + t^5.72 + 3*t^5.729 + t^5.991 + t^6.009 + 2*t^6.271 + t^6.28 + 3*t^6.541 + 3*t^6.551 + 3*t^6.821 + 3*t^7.092 + 2*t^7.101 + 3*t^7.362 + 3*t^7.372 + 3*t^7.633 + 2*t^7.642 + t^7.904 + 5*t^7.913 + t^7.922 + t^8.174 + t^8.184 + t^8.193 + t^8.445 - t^8.454 + 4*t^8.464 + t^8.715 + t^8.725 + 5*t^8.734 + t^8.986 - 2*t^8.995 - t^4.362/y - t^6.546/y - t^7.087/y - t^7.358/y + t^7.367/y + (2*t^7.638)/y + t^7.908/y + (3*t^8.179)/y + t^8.188/y + t^8.449/y + t^8.459/y + t^8.72/y + (2*t^8.729)/y - t^4.362*y - t^6.546*y - t^7.087*y - t^7.358*y + t^7.367*y + 2*t^7.638*y + t^7.908*y + 3*t^8.179*y + t^8.188*y + t^8.449*y + t^8.459*y + t^8.72*y + 2*t^8.729*y | g1^8*t^2.184 + t^2.454/g1^2 + t^2.725/g1^12 + t^2.995/g1^22 + g1^22*t^3.005 + 2*g1^2*t^3.546 + (2*t^3.816)/g1^8 + g1^26*t^4.096 + 3*g1^16*t^4.367 + g1^6*t^4.638 + (2*t^4.908)/g1^4 + g1^40*t^4.918 + (2*t^5.179)/g1^14 + g1^30*t^5.188 + g1^20*t^5.459 + t^5.72/g1^34 + 3*g1^10*t^5.729 + t^5.991/g1^44 + g1^44*t^6.009 + (2*t^6.271)/g1^10 + g1^34*t^6.28 + (3*t^6.541)/g1^20 + 3*g1^24*t^6.551 + 3*g1^14*t^6.821 + 3*g1^4*t^7.092 + 2*g1^48*t^7.101 + (3*t^7.362)/g1^6 + 3*g1^38*t^7.372 + (3*t^7.633)/g1^16 + 2*g1^28*t^7.642 + t^7.904/g1^26 + 5*g1^18*t^7.913 + g1^62*t^7.922 + t^8.174/g1^36 + g1^8*t^8.184 + g1^52*t^8.193 + t^8.445/g1^46 - t^8.454/g1^2 + 4*g1^42*t^8.464 + t^8.715/g1^56 + t^8.725/g1^12 + 5*g1^32*t^8.734 + t^8.986/g1^66 - (2*t^8.995)/g1^22 - t^4.362/(g1^6*y) - (g1^2*t^6.546)/y - t^7.087/(g1^18*y) - t^7.358/(g1^28*y) + (g1^16*t^7.367)/y + (2*g1^6*t^7.638)/y + t^7.908/(g1^4*y) + (3*t^8.179)/(g1^14*y) + (g1^30*t^8.188)/y + t^8.449/(g1^24*y) + (g1^20*t^8.459)/y + t^8.72/(g1^34*y) + (2*g1^10*t^8.729)/y - (t^4.362*y)/g1^6 - g1^2*t^6.546*y - (t^7.087*y)/g1^18 - (t^7.358*y)/g1^28 + g1^16*t^7.367*y + 2*g1^6*t^7.638*y + (t^7.908*y)/g1^4 + (3*t^8.179*y)/g1^14 + g1^30*t^8.188*y + (t^8.449*y)/g1^24 + g1^20*t^8.459*y + (t^8.72*y)/g1^34 + 2*g1^10*t^8.729*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 |
|---|---|---|---|---|---|---|---|---|---|
| 2639 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}M_{5}$ + ${ }M_{4}M_{7}$ | 0.6651 | 0.8251 | 0.8061 | [M:[0.9459, 0.8133, 0.9459, 0.8133, 1.1867, 0.7469, 1.1867], q:[0.6475, 0.4066], qb:[0.4066, 0.7801], phi:[0.4398]] | t^2.241 + t^2.44 + t^2.639 + 2*t^2.838 + 2*t^3.56 + 2*t^3.759 + t^4.283 + 3*t^4.482 + t^4.681 + 2*t^4.88 + 3*t^5.079 + t^5.204 + t^5.278 + 2*t^5.476 + 3*t^5.675 + 2*t^5.801 - t^6. - t^4.319/y - t^4.319*y | detail |