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 |
|---|---|---|---|---|---|---|---|---|---|
| 56707 | SU2adj1nf2 | ${}M_{1}\phi_{1}^{2}$ + ${ }M_{2}q_{1}q_{2}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}^{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{6}q_{1}\tilde{q}_{1}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{6}M_{7}$ | 0.606 | 0.7748 | 0.7821 | [M:[1.0215, 0.957, 1.0, 1.0215, 0.7446, 0.7231, 1.2769], q:[0.5215, 0.5215], qb:[0.7554, 0.2446], phi:[0.4892]] | [M:[[-4], [8], [0], [-4], [1], [5], [-5]], q:[[-4], [-4]], qb:[[-1], [1]], phi:[[2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{5}$, ${ }q_{1}\tilde{q}_{2}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{2}$, ${ }M_{3}$, ${ }M_{1}$, ${ }M_{4}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{7}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{5}^{2}$, ${ }M_{5}q_{1}\tilde{q}_{2}$, ${ }M_{5}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }q_{1}^{2}\tilde{q}_{2}^{2}$, ${ }q_{1}q_{2}\tilde{q}_{2}^{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{2}M_{5}$, ${ }M_{3}M_{5}$, ${ }M_{1}M_{5}$, ${ }M_{4}M_{5}$, ${ }M_{3}q_{1}\tilde{q}_{2}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }M_{1}q_{1}\tilde{q}_{2}$, ${ }M_{4}q_{1}\tilde{q}_{2}$, ${ }M_{1}q_{2}\tilde{q}_{2}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }M_{2}^{2}$, ${ }M_{2}M_{3}$, ${ }M_{1}M_{2}$, ${ }M_{2}M_{4}$ | ${}M_{5}\phi_{1}q_{2}\tilde{q}_{2}$ | -4 | t^2.234 + 2*t^2.298 + t^2.871 + t^3. + 2*t^3.065 + t^3.766 + 2*t^3.831 + t^4.468 + 2*t^4.532 + 6*t^4.597 + t^5.105 + t^5.234 + 4*t^5.298 + 4*t^5.363 + t^5.742 + t^5.871 + t^5.935 - 4*t^6. + 5*t^6.065 + 6*t^6.129 - t^6.637 + t^6.702 - t^6.766 + 6*t^6.831 + 12*t^6.895 + t^7.339 - t^7.468 + 8*t^7.597 + 12*t^7.661 + t^7.976 + t^8.105 + t^8.169 - 6*t^8.234 - 7*t^8.298 + 10*t^8.363 + 14*t^8.428 + t^8.613 + t^8.742 + t^8.806 - 3*t^8.871 + t^8.935 - t^4.468/y - t^6.702/y - t^7.339/y + t^7.403/y + t^7.532/y + (2*t^7.597)/y + t^8.105/y + (2*t^8.169)/y + (2*t^8.234)/y + (4*t^8.298)/y + (4*t^8.363)/y + t^8.871/y + t^8.935/y - t^4.468*y - t^6.702*y - t^7.339*y + t^7.403*y + t^7.532*y + 2*t^7.597*y + t^8.105*y + 2*t^8.169*y + 2*t^8.234*y + 4*t^8.298*y + 4*t^8.363*y + t^8.871*y + t^8.935*y | g1*t^2.234 + (2*t^2.298)/g1^3 + g1^8*t^2.871 + t^3. + (2*t^3.065)/g1^4 + t^3.766/g1 + (2*t^3.831)/g1^5 + g1^2*t^4.468 + (2*t^4.532)/g1^2 + (6*t^4.597)/g1^6 + g1^9*t^5.105 + g1*t^5.234 + (4*t^5.298)/g1^3 + (4*t^5.363)/g1^7 + g1^16*t^5.742 + g1^8*t^5.871 + g1^4*t^5.935 - 4*t^6. + (5*t^6.065)/g1^4 + (6*t^6.129)/g1^8 - g1^7*t^6.637 + g1^3*t^6.702 - t^6.766/g1 + (6*t^6.831)/g1^5 + (12*t^6.895)/g1^9 + g1^10*t^7.339 - g1^2*t^7.468 + (8*t^7.597)/g1^6 + (12*t^7.661)/g1^10 + g1^17*t^7.976 + g1^9*t^8.105 + g1^5*t^8.169 - 6*g1*t^8.234 - (7*t^8.298)/g1^3 + (10*t^8.363)/g1^7 + (14*t^8.428)/g1^11 + g1^24*t^8.613 + g1^16*t^8.742 + g1^12*t^8.806 - 3*g1^8*t^8.871 + g1^4*t^8.935 - (g1^2*t^4.468)/y - (g1^3*t^6.702)/y - (g1^10*t^7.339)/y + (g1^6*t^7.403)/y + t^7.532/(g1^2*y) + (2*t^7.597)/(g1^6*y) + (g1^9*t^8.105)/y + (2*g1^5*t^8.169)/y + (2*g1*t^8.234)/y + (4*t^8.298)/(g1^3*y) + (4*t^8.363)/(g1^7*y) + (g1^8*t^8.871)/y + (g1^4*t^8.935)/y - g1^2*t^4.468*y - g1^3*t^6.702*y - g1^10*t^7.339*y + g1^6*t^7.403*y + (t^7.532*y)/g1^2 + (2*t^7.597*y)/g1^6 + g1^9*t^8.105*y + 2*g1^5*t^8.169*y + 2*g1*t^8.234*y + (4*t^8.298*y)/g1^3 + (4*t^8.363*y)/g1^7 + g1^8*t^8.871*y + g1^4*t^8.935*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 |
|---|---|---|---|---|---|---|---|---|---|
| 55019 | SU2adj1nf2 | ${}M_{1}\phi_{1}^{2}$ + ${ }M_{2}q_{1}q_{2}$ + ${ }\phi_{1}\tilde{q}_{1}^{2}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}^{2}$ + ${ }M_{4}\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{5}\phi_{1}q_{1}\tilde{q}_{2}$ + ${ }M_{6}q_{1}\tilde{q}_{1}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ | 0.6261 | 0.8118 | 0.7712 | [M:[1.0287, 0.9427, 1.0, 1.0287, 0.7428, 0.7142], q:[0.5287, 0.5287], qb:[0.7572, 0.2428], phi:[0.4857]] | t^2.143 + t^2.229 + 2*t^2.314 + t^2.828 + t^3. + 2*t^3.086 + t^3.771 + t^3.857 + t^4.285 + t^4.371 + 3*t^4.457 + 2*t^4.543 + 6*t^4.629 + t^4.971 + t^5.057 + t^5.143 + 3*t^5.229 + 4*t^5.314 + 4*t^5.4 + t^5.656 + t^5.828 + 2*t^5.914 - 3*t^6. - t^4.457/y - t^4.457*y | detail |