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 |
|---|---|---|---|---|---|---|---|---|---|
| 2610 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{2}M_{3}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}M_{7}$ | 0.64 | 0.7978 | 0.8023 | [M:[1.0144, 0.8894, 1.1106, 0.7933, 1.2067, 0.7308, 1.1106], q:[0.5409, 0.4447], qb:[0.3485, 0.762], phi:[0.476]] | [M:[[-38], [14], [-14], [-10], [10], [16], [-14]], q:[[31], [7]], qb:[[-17], [3]], phi:[[-6]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{6}$, ${ }M_{4}$, ${ }\phi_{1}^{2}$, ${ }M_{1}$, ${ }M_{3}$, ${ }M_{7}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{5}$, ${ }q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{6}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }M_{4}M_{6}$, ${ }\phi_{1}q_{1}^{2}$, ${ }M_{4}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{1}M_{6}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{6}M_{7}$, ${ }M_{3}M_{4}$, ${ }M_{4}M_{7}$, ${ }\phi_{1}^{4}$, ${ }M_{6}\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{5}M_{6}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$ | ${}$ | -2 | t^2.192 + t^2.38 + t^2.856 + t^3.043 + 2*t^3.332 + t^3.519 + t^3.62 + t^3.909 + 2*t^4.096 + 2*t^4.385 + t^4.572 + t^4.673 + t^4.76 + t^5.048 + 2*t^5.236 + 2*t^5.524 + 2*t^5.711 + t^5.813 + 2*t^5.899 - 2*t^6. + t^6.086 + t^6.101 + t^6.187 + 3*t^6.375 + t^6.476 + t^6.562 + t^6.577 + 2*t^6.663 + t^6.764 + t^6.851 + t^6.866 + 4*t^6.952 + t^7.038 + t^7.139 + 2*t^7.24 + 4*t^7.428 + t^7.529 + 2*t^7.615 + 3*t^7.716 + t^7.904 + 3*t^8.005 + 3*t^8.091 - t^8.192 + 2*t^8.279 + 2*t^8.293 - t^8.38 + 3*t^8.567 + t^8.582 - t^8.668 + 2*t^8.755 + 3*t^8.769 + t^8.942 - t^4.428/y - t^6.62/y + t^7.096/y - t^7.284/y + t^7.385/y - t^7.471/y + (2*t^7.572)/y - t^7.76/y + t^8.048/y + (3*t^8.236)/y + t^8.423/y + (2*t^8.524)/y + (3*t^8.711)/y + (2*t^8.899)/y - t^4.428*y - t^6.62*y + t^7.096*y - t^7.284*y + t^7.385*y - t^7.471*y + 2*t^7.572*y - t^7.76*y + t^8.048*y + 3*t^8.236*y + t^8.423*y + 2*t^8.524*y + 3*t^8.711*y + 2*t^8.899*y | g1^16*t^2.192 + t^2.38/g1^10 + t^2.856/g1^12 + t^3.043/g1^38 + (2*t^3.332)/g1^14 + t^3.519/g1^40 + g1^10*t^3.62 + g1^34*t^3.909 + 2*g1^8*t^4.096 + 2*g1^32*t^4.385 + g1^6*t^4.572 + g1^56*t^4.673 + t^4.76/g1^20 + g1^4*t^5.048 + (2*t^5.236)/g1^22 + 2*g1^2*t^5.524 + (2*t^5.711)/g1^24 + g1^26*t^5.813 + (2*t^5.899)/g1^50 - 2*t^6. + t^6.086/g1^76 + g1^50*t^6.101 + t^6.187/g1^26 + (3*t^6.375)/g1^52 + t^6.476/g1^2 + t^6.562/g1^78 + g1^48*t^6.577 + (2*t^6.663)/g1^28 + g1^22*t^6.764 + t^6.851/g1^54 + g1^72*t^6.866 + (4*t^6.952)/g1^4 + t^7.038/g1^80 + t^7.139/g1^30 + 2*g1^20*t^7.24 + (4*t^7.428)/g1^6 + g1^44*t^7.529 + (2*t^7.615)/g1^32 + 3*g1^18*t^7.716 + t^7.904/g1^8 + 3*g1^42*t^8.005 + (3*t^8.091)/g1^34 - g1^16*t^8.192 + (2*t^8.279)/g1^60 + 2*g1^66*t^8.293 - t^8.38/g1^10 + (3*t^8.567)/g1^36 + g1^90*t^8.582 - g1^14*t^8.668 + (2*t^8.755)/g1^62 + 3*g1^64*t^8.769 + t^8.942/g1^88 - t^4.428/(g1^6*y) - (g1^10*t^6.62)/y + (g1^8*t^7.096)/y - t^7.284/(g1^18*y) + (g1^32*t^7.385)/y - t^7.471/(g1^44*y) + (2*g1^6*t^7.572)/y - t^7.76/(g1^20*y) + (g1^4*t^8.048)/y + (3*t^8.236)/(g1^22*y) + t^8.423/(g1^48*y) + (2*g1^2*t^8.524)/y + (3*t^8.711)/(g1^24*y) + (2*t^8.899)/(g1^50*y) - (t^4.428*y)/g1^6 - g1^10*t^6.62*y + g1^8*t^7.096*y - (t^7.284*y)/g1^18 + g1^32*t^7.385*y - (t^7.471*y)/g1^44 + 2*g1^6*t^7.572*y - (t^7.76*y)/g1^20 + g1^4*t^8.048*y + (3*t^8.236*y)/g1^22 + (t^8.423*y)/g1^48 + 2*g1^2*t^8.524*y + (3*t^8.711*y)/g1^24 + (2*t^8.899*y)/g1^50 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 1522 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{4}M_{5}$ + ${ }\phi_{1}\tilde{q}_{2}^{2}$ + ${ }M_{2}M_{3}$ + ${ }M_{6}\phi_{1}q_{2}\tilde{q}_{1}$ | 0.6503 | 0.8152 | 0.7977 | [M:[1.0329, 0.8826, 1.1174, 0.7981, 1.2019, 0.723], q:[0.5258, 0.4413], qb:[0.3568, 0.7606], phi:[0.4789]] | t^2.169 + t^2.394 + t^2.648 + t^2.873 + t^3.099 + t^3.352 + t^3.578 + t^3.606 + t^3.859 + 2*t^4.084 + 2*t^4.338 + t^4.563 + t^4.591 + t^4.789 + t^4.817 + 2*t^5.042 + 2*t^5.268 + t^5.296 + 2*t^5.521 + 2*t^5.747 + t^5.775 + 2*t^5.972 - t^6. - t^4.437/y - t^4.437*y | detail |