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 |
|---|---|---|---|---|---|---|---|---|---|
| 58227 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{5}$ + ${ }M_{1}M_{6}$ + ${ }M_{2}M_{7}$ + ${ }M_{8}\phi_{1}q_{1}q_{2}$ | 0.6632 | 0.8397 | 0.7897 | [M:[1.2044, 0.8175, 0.7956, 0.7883, 0.7956, 0.7956, 1.1825, 0.8029], q:[0.3942, 0.4015], qb:[0.7883, 0.8102], phi:[0.4015]] | [M:[[3], [12], [-3], [-8], [-3], [-3], [-12], [2]], q:[[-4], [1]], qb:[[-8], [7]], phi:[[1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }M_{3}$, ${ }M_{5}$, ${ }M_{6}$, ${ }M_{8}$, ${ }\phi_{1}^{2}$, ${ }M_{7}$, ${ }\phi_{1}q_{1}^{2}$, ${ }q_{2}\tilde{q}_{1}$, ${ }M_{4}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}M_{5}$, ${ }M_{4}M_{6}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{3}^{2}$, ${ }M_{3}M_{5}$, ${ }M_{5}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{5}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{4}M_{8}$, ${ }M_{4}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{3}M_{8}$, ${ }M_{5}M_{8}$, ${ }M_{6}M_{8}$, ${ }M_{3}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{8}^{2}$, ${ }M_{8}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{4}M_{7}$, ${ }M_{3}M_{7}$, ${ }M_{5}M_{7}$, ${ }M_{6}M_{7}$, ${ }M_{4}\phi_{1}q_{1}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{7}M_{8}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{5}\phi_{1}q_{1}^{2}$, ${ }M_{6}\phi_{1}q_{1}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }M_{6}q_{2}\tilde{q}_{1}$, ${ }M_{8}\phi_{1}q_{1}^{2}$, ${ }\phi_{1}^{3}q_{1}^{2}$, ${ }M_{8}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$ | ${}$ | -3 | t^2.365 + 3*t^2.387 + 2*t^2.409 + t^3.548 + 2*t^3.569 + t^4.73 + 3*t^4.752 + 8*t^4.774 + 7*t^4.796 + 3*t^4.817 + t^5.913 + 5*t^5.934 + 7*t^5.956 + 2*t^5.978 - 3*t^6. - 2*t^6.022 - t^6.044 + 2*t^7.095 + 5*t^7.117 + 10*t^7.139 + 14*t^7.161 + 13*t^7.183 + 7*t^7.204 + t^7.226 - t^7.248 + t^8.278 + 5*t^8.299 + 13*t^8.321 + 17*t^8.343 + 4*t^8.365 - 11*t^8.387 - 14*t^8.409 - 8*t^8.431 - 2*t^8.452 - t^4.204/y - t^6.569/y - (2*t^6.591)/y - (2*t^6.613)/y + (3*t^7.752)/y + (5*t^7.774)/y + (8*t^7.796)/y + (3*t^7.817)/y + t^7.839/y + t^8.913/y + (4*t^8.934)/y + (6*t^8.956)/y - t^8.978/y - t^4.204*y - t^6.569*y - 2*t^6.591*y - 2*t^6.613*y + 3*t^7.752*y + 5*t^7.774*y + 8*t^7.796*y + 3*t^7.817*y + t^7.839*y + t^8.913*y + 4*t^8.934*y + 6*t^8.956*y - t^8.978*y | t^2.365/g1^8 + (3*t^2.387)/g1^3 + 2*g1^2*t^2.409 + t^3.548/g1^12 + (2*t^3.569)/g1^7 + t^4.73/g1^16 + (3*t^4.752)/g1^11 + (8*t^4.774)/g1^6 + (7*t^4.796)/g1 + 3*g1^4*t^4.817 + t^5.913/g1^20 + (5*t^5.934)/g1^15 + (7*t^5.956)/g1^10 + (2*t^5.978)/g1^5 - 3*t^6. - 2*g1^5*t^6.022 - g1^10*t^6.044 + (2*t^7.095)/g1^24 + (5*t^7.117)/g1^19 + (10*t^7.139)/g1^14 + (14*t^7.161)/g1^9 + (13*t^7.183)/g1^4 + 7*g1*t^7.204 + g1^6*t^7.226 - g1^11*t^7.248 + t^8.278/g1^28 + (5*t^8.299)/g1^23 + (13*t^8.321)/g1^18 + (17*t^8.343)/g1^13 + (4*t^8.365)/g1^8 - (11*t^8.387)/g1^3 - 14*g1^2*t^8.409 - 8*g1^7*t^8.431 - 2*g1^12*t^8.452 - (g1*t^4.204)/y - t^6.569/(g1^7*y) - (2*t^6.591)/(g1^2*y) - (2*g1^3*t^6.613)/y + (3*t^7.752)/(g1^11*y) + (5*t^7.774)/(g1^6*y) + (8*t^7.796)/(g1*y) + (3*g1^4*t^7.817)/y + (g1^9*t^7.839)/y + t^8.913/(g1^20*y) + (4*t^8.934)/(g1^15*y) + (6*t^8.956)/(g1^10*y) - t^8.978/(g1^5*y) - g1*t^4.204*y - (t^6.569*y)/g1^7 - (2*t^6.591*y)/g1^2 - 2*g1^3*t^6.613*y + (3*t^7.752*y)/g1^11 + (5*t^7.774*y)/g1^6 + (8*t^7.796*y)/g1 + 3*g1^4*t^7.817*y + g1^9*t^7.839*y + (t^8.913*y)/g1^20 + (4*t^8.934*y)/g1^15 + (6*t^8.956*y)/g1^10 - (t^8.978*y)/g1^5 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 56080 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}q_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{5}\phi_{1}q_{2}^{2}$ + ${ }M_{1}M_{5}$ + ${ }M_{1}M_{6}$ + ${ }M_{2}M_{7}$ | 0.6469 | 0.8121 | 0.7965 | [M:[1.2069, 0.8276, 0.7931, 0.7816, 0.7931, 0.7931, 1.1724], q:[0.3908, 0.4023], qb:[0.7816, 0.8161], phi:[0.4023]] | t^2.345 + 3*t^2.379 + t^2.414 + t^3.517 + 2*t^3.552 + t^3.586 + t^4.69 + 3*t^4.724 + 7*t^4.759 + 4*t^4.793 + t^4.828 + t^5.862 + 5*t^5.896 + 7*t^5.931 + 3*t^5.965 - 2*t^6. - t^4.207/y - t^4.207*y | detail |