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 |
|---|---|---|---|---|---|---|---|---|---|
| 2892 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{6}q_{1}\tilde{q}_{1}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{2}$ | 0.625 | 0.8101 | 0.7715 | [M:[1.0, 1.0193, 0.9615, 1.0193, 0.7548, 0.7356], q:[0.7548, 0.2452], qb:[0.5096, 0.5289], phi:[0.4904]] | [M:[[0], [4], [-8], [4], [1], [-3]], q:[[1], [-1]], qb:[[2], [6]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{6}$, ${ }M_{5}$, ${ }q_{2}\tilde{q}_{1}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{3}$, ${ }M_{1}$, ${ }M_{2}$, ${ }M_{4}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }q_{1}\tilde{q}_{2}$, ${ }M_{6}^{2}$, ${ }M_{5}M_{6}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{6}q_{2}\tilde{q}_{1}$, ${ }M_{5}^{2}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }M_{6}q_{2}\tilde{q}_{2}$, ${ }M_{5}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{3}M_{5}$, ${ }M_{1}M_{6}$, ${ }M_{1}M_{5}$, ${ }M_{2}M_{6}$, ${ }M_{4}M_{6}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{2}M_{5}$, ${ }M_{4}M_{5}$, ${ }M_{2}q_{2}\tilde{q}_{1}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{2}q_{2}\tilde{q}_{2}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }M_{3}^{2}$, ${ }M_{1}M_{3}$ | ${}$ | -2 | t^2.207 + 2*t^2.264 + t^2.322 + t^2.884 + t^3. + 2*t^3.058 + t^3.793 + t^3.851 + t^4.413 + 2*t^4.471 + 5*t^4.529 + 3*t^4.587 + 2*t^4.644 + t^5.091 + t^5.149 + t^5.207 + 4*t^5.264 + 5*t^5.322 + 2*t^5.38 + t^5.769 + t^5.884 - 2*t^6. + 3*t^6.058 + 5*t^6.116 + t^6.173 + t^6.678 + 3*t^6.736 + 6*t^6.793 + 8*t^6.851 + 6*t^6.909 + 2*t^6.967 + t^7.298 + t^7.356 + 2*t^7.413 + t^7.471 + 5*t^7.529 + 10*t^7.587 + 7*t^7.644 + 4*t^7.702 + t^7.975 + t^8.033 + t^8.091 + t^8.149 - 4*t^8.207 - 6*t^8.264 + 3*t^8.322 + 9*t^8.38 + 6*t^8.438 + 2*t^8.496 + t^8.653 + t^8.769 + t^8.827 - 2*t^8.884 + t^8.942 - t^4.471/y - t^6.678/y - t^6.736/y - t^7.356/y + t^7.413/y + (2*t^7.471)/y + t^7.529/y + (3*t^7.587)/y + t^8.091/y + (2*t^8.149)/y + (3*t^8.207)/y + (5*t^8.264)/y + (5*t^8.322)/y + (2*t^8.38)/y + t^8.942/y - t^4.471*y - t^6.678*y - t^6.736*y - t^7.356*y + t^7.413*y + 2*t^7.471*y + t^7.529*y + 3*t^7.587*y + t^8.091*y + 2*t^8.149*y + 3*t^8.207*y + 5*t^8.264*y + 5*t^8.322*y + 2*t^8.38*y + t^8.942*y | t^2.207/g1^3 + 2*g1*t^2.264 + g1^5*t^2.322 + t^2.884/g1^8 + t^3. + 2*g1^4*t^3.058 + g1^3*t^3.793 + g1^7*t^3.851 + t^4.413/g1^6 + (2*t^4.471)/g1^2 + 5*g1^2*t^4.529 + 3*g1^6*t^4.587 + 2*g1^10*t^4.644 + t^5.091/g1^11 + t^5.149/g1^7 + t^5.207/g1^3 + 4*g1*t^5.264 + 5*g1^5*t^5.322 + 2*g1^9*t^5.38 + t^5.769/g1^16 + t^5.884/g1^8 - 2*t^6. + 3*g1^4*t^6.058 + 5*g1^8*t^6.116 + g1^12*t^6.173 + t^6.678/g1^5 + (3*t^6.736)/g1 + 6*g1^3*t^6.793 + 8*g1^7*t^6.851 + 6*g1^11*t^6.909 + 2*g1^15*t^6.967 + t^7.298/g1^14 + t^7.356/g1^10 + (2*t^7.413)/g1^6 + t^7.471/g1^2 + 5*g1^2*t^7.529 + 10*g1^6*t^7.587 + 7*g1^10*t^7.644 + 4*g1^14*t^7.702 + t^7.975/g1^19 + t^8.033/g1^15 + t^8.091/g1^11 + t^8.149/g1^7 - (4*t^8.207)/g1^3 - 6*g1*t^8.264 + 3*g1^5*t^8.322 + 9*g1^9*t^8.38 + 6*g1^13*t^8.438 + 2*g1^17*t^8.496 + t^8.653/g1^24 + t^8.769/g1^16 + t^8.827/g1^12 - (2*t^8.884)/g1^8 + t^8.942/g1^4 - t^4.471/(g1^2*y) - t^6.678/(g1^5*y) - t^6.736/(g1*y) - t^7.356/(g1^10*y) + t^7.413/(g1^6*y) + (2*t^7.471)/(g1^2*y) + (g1^2*t^7.529)/y + (3*g1^6*t^7.587)/y + t^8.091/(g1^11*y) + (2*t^8.149)/(g1^7*y) + (3*t^8.207)/(g1^3*y) + (5*g1*t^8.264)/y + (5*g1^5*t^8.322)/y + (2*g1^9*t^8.38)/y + t^8.942/(g1^4*y) - (t^4.471*y)/g1^2 - (t^6.678*y)/g1^5 - (t^6.736*y)/g1 - (t^7.356*y)/g1^10 + (t^7.413*y)/g1^6 + (2*t^7.471*y)/g1^2 + g1^2*t^7.529*y + 3*g1^6*t^7.587*y + (t^8.091*y)/g1^11 + (2*t^8.149*y)/g1^7 + (3*t^8.207*y)/g1^3 + 5*g1*t^8.264*y + 5*g1^5*t^8.322*y + 2*g1^9*t^8.38*y + (t^8.942*y)/g1^4 |
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 |
|---|---|---|---|---|---|---|---|---|
| 3464 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{6}q_{1}\tilde{q}_{1}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{6}M_{7}$ | 0.6055 | 0.7749 | 0.7813 | [M:[1.0, 1.0141, 0.9717, 1.0141, 0.7535, 0.7394, 1.2606], q:[0.7535, 0.2465], qb:[0.5071, 0.5212], phi:[0.4929]] | 2*t^2.261 + t^2.303 + t^2.915 + t^3. + 2*t^3.042 + 2*t^3.782 + t^3.824 + 4*t^4.521 + 3*t^4.564 + 2*t^4.606 + t^5.176 + 2*t^5.261 + 5*t^5.303 + 2*t^5.345 + t^5.83 + t^5.915 - 3*t^6. - t^4.479/y - t^4.479*y | detail | |
| 3465 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{6}q_{1}\tilde{q}_{1}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{2}$ + ${ }M_{7}\phi_{1}q_{2}\tilde{q}_{2}$ | 0.6447 | 0.8459 | 0.7621 | [M:[1.0, 1.0239, 0.9521, 1.0239, 0.756, 0.732, 0.732], q:[0.756, 0.244], qb:[0.512, 0.5359], phi:[0.488]] | 2*t^2.196 + 2*t^2.268 + t^2.34 + t^2.856 + t^3. + 2*t^3.072 + t^3.876 + 3*t^4.392 + 4*t^4.464 + 6*t^4.536 + 3*t^4.608 + 2*t^4.68 + 2*t^5.052 + t^5.124 + 2*t^5.196 + 6*t^5.268 + 5*t^5.34 + 2*t^5.412 + t^5.713 + t^5.856 - 3*t^6. - t^4.464/y - t^4.464*y | detail |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 1878 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}^{2}$ + ${ }M_{4}\phi_{1}q_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{6}q_{1}\tilde{q}_{1}$ | 0.6266 | 0.8144 | 0.7694 | [M:[1.0, 1.0266, 0.9468, 1.0266, 0.7278, 0.7012], q:[0.7567, 0.2433], qb:[0.5421, 0.5111], phi:[0.4867]] | t^2.104 + t^2.183 + t^2.263 + t^2.356 + t^2.84 + t^3. + 2*t^3.08 + t^3.723 + t^3.803 + t^4.207 + t^4.287 + 2*t^4.367 + t^4.447 + t^4.46 + 2*t^4.527 + t^4.54 + 2*t^4.62 + 2*t^4.713 + t^4.944 + t^5.024 + t^5.104 + 3*t^5.183 + 3*t^5.263 + 2*t^5.343 + t^5.356 + 2*t^5.436 + t^5.681 + t^5.827 + t^5.84 + t^5.907 + t^5.92 + 2*t^5.987 - 3*t^6. - t^4.46/y - t^4.46*y | detail |