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 |
|---|---|---|---|---|---|---|---|---|---|
| 1905 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}M_{4}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ | 0.5952 | 0.7742 | 0.7687 | [M:[0.9324, 1.2029, 1.0676, 0.7971, 0.8043], q:[0.7331, 0.3345], qb:[0.3345, 0.4626], phi:[0.5338]] | [M:[[4], [-12], [-4], [12], [-18]], q:[[1], [-5]], qb:[[-5], [17]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}q_{2}\tilde{q}_{1}$, ${ }M_{4}$, ${ }q_{2}\tilde{q}_{2}$, ${ }M_{5}$, ${ }M_{3}$, ${ }\phi_{1}^{2}$, ${ }q_{1}\tilde{q}_{1}$, ${ }M_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{1}$, ${ }q_{2}^{2}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{5}q_{2}\tilde{q}_{1}$, ${ }M_{4}^{2}$, ${ }M_{4}q_{2}\tilde{q}_{2}$, ${ }q_{2}^{2}\tilde{q}_{2}^{2}$, ${ }M_{4}M_{5}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }M_{5}q_{2}\tilde{q}_{2}$, ${ }M_{5}^{2}$, ${ }M_{3}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{1}$, ${ }q_{1}q_{2}\tilde{q}_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{4}q_{1}\tilde{q}_{1}$, ${ }M_{3}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}^{2}q_{2}\tilde{q}_{2}$, ${ }M_{3}M_{5}$, ${ }M_{5}\phi_{1}^{2}$, ${ }M_{5}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}^{3}$ | ${}M_{4}\phi_{1}q_{2}^{2}$, ${ }M_{4}\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{2}^{3}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}^{2}\tilde{q}_{2}$ | 1 | t^2.007 + 2*t^2.391 + t^2.413 + 3*t^3.203 + 3*t^3.609 + 2*t^3.993 + t^4.014 + t^4.377 + 2*t^4.399 + t^4.42 + 3*t^4.783 + 2*t^4.804 + t^4.826 + 3*t^5.21 + 5*t^5.594 + 4*t^5.616 + t^6. + 4*t^6.022 + 2*t^6.384 + 5*t^6.406 + t^6.427 + 2*t^6.768 + t^6.79 + 8*t^6.811 + t^6.833 + 3*t^7.174 + 3*t^7.196 + 8*t^7.217 + t^7.239 + t^7.58 + 3*t^7.601 + 4*t^7.623 + 7*t^7.986 + 2*t^8.007 + 5*t^8.029 + 2*t^8.37 - 3*t^8.391 + 4*t^8.413 + 4*t^8.434 + t^8.754 + 2*t^8.776 + 3*t^8.797 + 6*t^8.819 + t^8.84 - t^4.601/y - t^7.014/y + (3*t^7.399)/y + t^7.42/y + t^7.783/y + t^7.804/y + t^8.189/y + (3*t^8.21)/y + (6*t^8.594)/y + (6*t^8.616)/y - t^4.601*y - t^7.014*y + 3*t^7.399*y + t^7.42*y + t^7.783*y + t^7.804*y + t^8.189*y + 3*t^8.21*y + 6*t^8.594*y + 6*t^8.616*y | t^2.007/g1^10 + 2*g1^12*t^2.391 + t^2.413/g1^18 + (3*t^3.203)/g1^4 + (3*t^3.609)/g1^12 + 2*g1^10*t^3.993 + t^4.014/g1^20 + g1^32*t^4.377 + 2*g1^2*t^4.399 + t^4.42/g1^28 + 3*g1^24*t^4.783 + (2*t^4.804)/g1^6 + t^4.826/g1^36 + (3*t^5.21)/g1^14 + 5*g1^8*t^5.594 + (4*t^5.616)/g1^22 + t^6. + (4*t^6.022)/g1^30 + 2*g1^22*t^6.384 + (5*t^6.406)/g1^8 + t^6.427/g1^38 + 2*g1^44*t^6.768 + g1^14*t^6.79 + (8*t^6.811)/g1^16 + t^6.833/g1^46 + 3*g1^36*t^7.174 + 3*g1^6*t^7.196 + (8*t^7.217)/g1^24 + t^7.239/g1^54 + g1^28*t^7.58 + (3*t^7.601)/g1^2 + (4*t^7.623)/g1^32 + 7*g1^20*t^7.986 + (2*t^8.007)/g1^10 + (5*t^8.029)/g1^40 + 2*g1^42*t^8.37 - 3*g1^12*t^8.391 + (4*t^8.413)/g1^18 + (4*t^8.434)/g1^48 + g1^64*t^8.754 + 2*g1^34*t^8.776 + 3*g1^4*t^8.797 + (6*t^8.819)/g1^26 + t^8.84/g1^56 - t^4.601/(g1^2*y) - t^7.014/(g1^20*y) + (3*g1^2*t^7.399)/y + t^7.42/(g1^28*y) + (g1^24*t^7.783)/y + t^7.804/(g1^6*y) + (g1^16*t^8.189)/y + (3*t^8.21)/(g1^14*y) + (6*g1^8*t^8.594)/y + (6*t^8.616)/(g1^22*y) - (t^4.601*y)/g1^2 - (t^7.014*y)/g1^20 + 3*g1^2*t^7.399*y + (t^7.42*y)/g1^28 + g1^24*t^7.783*y + (t^7.804*y)/g1^6 + g1^16*t^8.189*y + (3*t^8.21*y)/g1^14 + 6*g1^8*t^8.594*y + (6*t^8.616*y)/g1^22 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 543 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }\phi_{1}q_{1}^{2}$ + ${ }M_{1}\phi_{1}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{4}\phi_{1}q_{2}\tilde{q}_{1}$ + ${ }M_{2}M_{4}$ | 0.5799 | 0.7477 | 0.7755 | [M:[0.9257, 1.223, 1.0743, 0.777], q:[0.7314, 0.3429], qb:[0.3429, 0.4341], phi:[0.5372]] | t^2.057 + 2*t^2.331 + 3*t^3.223 + t^3.497 + 3*t^3.669 + 2*t^3.943 + t^4.115 + t^4.216 + 2*t^4.389 + 3*t^4.662 + 3*t^5.28 + 6*t^5.554 + t^5.726 + 2*t^5.828 + t^6. - t^4.611/y - t^4.611*y | detail |