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 |
|---|---|---|---|---|---|---|---|---|---|
| 3553 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }\phi_{1}q_{2}^{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{7}\phi_{1}q_{1}\tilde{q}_{1}$ | 0.6687 | 0.8414 | 0.7947 | [M:[0.8238, 1.0587, 1.1762, 0.7063, 1.0587, 1.0595, 0.7056], q:[0.4115, 0.7647], qb:[0.4123, 0.529], phi:[0.4706]] | [M:[[-12], [4], [12], [-20], [4], [-30], [14]], q:[[11], [1]], qb:[[-23], [19]], phi:[[-2]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{7}$, ${ }M_{4}$, ${ }M_{1}$, ${ }M_{2}$, ${ }M_{5}$, ${ }M_{6}$, ${ }M_{3}$, ${ }q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }M_{7}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }M_{4}M_{7}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }M_{4}^{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }M_{1}M_{7}$, ${ }M_{1}M_{4}$, ${ }M_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{2}M_{7}$, ${ }M_{5}M_{7}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }M_{2}M_{4}$, ${ }M_{4}M_{5}$, ${ }M_{6}M_{7}$, ${ }M_{4}M_{6}$, ${ }M_{3}M_{7}$, ${ }M_{1}M_{2}$, ${ }M_{3}M_{4}$, ${ }M_{1}M_{5}$, ${ }M_{7}q_{2}\tilde{q}_{1}$, ${ }M_{1}M_{6}$, ${ }M_{4}q_{2}\tilde{q}_{1}$ | ${}M_{4}\phi_{1}q_{1}^{2}$ | -1 | t^2.117 + t^2.119 + t^2.471 + 2*t^3.176 + t^3.178 + t^3.529 + t^3.531 + t^3.881 + t^3.886 + 2*t^4.233 + 2*t^4.236 + t^4.238 + t^4.586 + t^4.588 + t^4.59 + t^4.943 + 2*t^5.293 + 3*t^5.295 + t^5.297 + t^5.645 + 3*t^5.648 + t^5.65 - t^6. + t^6.002 + t^6.005 + t^6.35 + 4*t^6.352 + 3*t^6.355 + 3*t^6.357 + t^6.703 + 3*t^6.705 + 3*t^6.707 + 2*t^6.709 + t^7.057 + 2*t^7.062 + t^7.064 + 3*t^7.41 + 3*t^7.412 + 4*t^7.414 + 2*t^7.416 + 2*t^7.762 + 3*t^7.764 + 3*t^7.767 + t^7.769 + t^7.771 + t^8.114 - 3*t^8.117 + 2*t^8.121 + t^8.124 + 2*t^8.467 + t^8.469 + 4*t^8.471 + 5*t^8.474 + 3*t^8.476 + 2*t^8.819 + 3*t^8.822 + 4*t^8.824 + 3*t^8.826 + 3*t^8.828 - t^4.412/y - t^6.529/y - t^6.531/y + t^7.233/y + (2*t^7.236)/y + (3*t^8.293)/y + (4*t^8.295)/y + t^8.297/y + (3*t^8.648)/y + t^8.65/y + t^8.998/y - t^4.412*y - t^6.529*y - t^6.531*y + t^7.233*y + 2*t^7.236*y + 3*t^8.293*y + 4*t^8.295*y + t^8.297*y + 3*t^8.648*y + t^8.65*y + t^8.998*y | g1^14*t^2.117 + t^2.119/g1^20 + t^2.471/g1^12 + 2*g1^4*t^3.176 + t^3.178/g1^30 + g1^12*t^3.529 + t^3.531/g1^22 + g1^20*t^3.881 + t^3.886/g1^48 + 2*g1^28*t^4.233 + (2*t^4.236)/g1^6 + t^4.238/g1^40 + g1^36*t^4.586 + g1^2*t^4.588 + t^4.59/g1^32 + t^4.943/g1^24 + 2*g1^18*t^5.293 + (3*t^5.295)/g1^16 + t^5.297/g1^50 + g1^26*t^5.645 + (3*t^5.648)/g1^8 + t^5.65/g1^42 - t^6. + t^6.002/g1^34 + t^6.005/g1^68 + g1^42*t^6.35 + 4*g1^8*t^6.352 + (3*t^6.355)/g1^26 + (3*t^6.357)/g1^60 + g1^50*t^6.703 + 3*g1^16*t^6.705 + (3*t^6.707)/g1^18 + (2*t^6.709)/g1^52 + g1^24*t^7.057 + (2*t^7.062)/g1^44 + t^7.064/g1^78 + 3*g1^32*t^7.41 + (3*t^7.412)/g1^2 + (4*t^7.414)/g1^36 + (2*t^7.416)/g1^70 + 2*g1^40*t^7.762 + 3*g1^6*t^7.764 + (3*t^7.767)/g1^28 + t^7.769/g1^62 + t^7.771/g1^96 + g1^48*t^8.114 - 3*g1^14*t^8.117 + (2*t^8.121)/g1^54 + t^8.124/g1^88 + 2*g1^56*t^8.467 + g1^22*t^8.469 + (4*t^8.471)/g1^12 + (5*t^8.474)/g1^46 + (3*t^8.476)/g1^80 + 2*g1^64*t^8.819 + 3*g1^30*t^8.822 + (4*t^8.824)/g1^4 + (3*t^8.826)/g1^38 + (3*t^8.828)/g1^72 - t^4.412/(g1^2*y) - (g1^12*t^6.529)/y - t^6.531/(g1^22*y) + (g1^28*t^7.233)/y + (2*t^7.236)/(g1^6*y) + (3*g1^18*t^8.293)/y + (4*t^8.295)/(g1^16*y) + t^8.297/(g1^50*y) + (3*t^8.648)/(g1^8*y) + t^8.65/(g1^42*y) + (g1^34*t^8.998)/y - (t^4.412*y)/g1^2 - g1^12*t^6.529*y - (t^6.531*y)/g1^22 + g1^28*t^7.233*y + (2*t^7.236*y)/g1^6 + 3*g1^18*t^8.293*y + (4*t^8.295*y)/g1^16 + (t^8.297*y)/g1^50 + (3*t^8.648*y)/g1^8 + (t^8.65*y)/g1^42 + g1^34*t^8.998*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 |
|---|---|---|---|---|---|---|---|---|---|
| 2961 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{5}\phi_{1}^{2}$ + ${ }\phi_{1}q_{2}^{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ | 0.6483 | 0.8029 | 0.8074 | [M:[0.8221, 1.0593, 1.1779, 0.7034, 1.0593, 1.0551], q:[0.4131, 0.7648], qb:[0.4089, 0.5317], phi:[0.4703]] | t^2.11 + t^2.466 + t^3.165 + 2*t^3.178 + t^3.521 + t^3.534 + t^3.865 + t^3.877 + t^3.89 + t^4.221 + t^4.233 + t^4.246 + t^4.576 + t^4.602 + t^4.932 + t^5.276 + 2*t^5.288 + t^5.632 + 2*t^5.644 + t^5.975 + t^5.987 - t^6. - t^4.411/y - t^4.411*y | detail |