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 |
|---|---|---|---|---|---|---|---|---|---|
| 56735 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{3}^{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{1}M_{5}$ + ${ }M_{5}M_{7}$ | 0.712 | 0.8818 | 0.8075 | [M:[0.9215, 1.0392, 1.0, 0.8823, 1.0785, 0.8431, 0.9215], q:[0.4412, 0.6373], qb:[0.5196, 0.4804], phi:[0.4804]] | [M:[[4], [-2], [0], [6], [-4], [8], [4]], q:[[3], [-7]], qb:[[-1], [1]], phi:[[1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{6}$, ${ }M_{4}$, ${ }M_{1}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }M_{6}^{2}$, ${ }M_{4}M_{6}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{1}M_{6}$, ${ }M_{6}M_{7}$, ${ }M_{1}M_{4}$, ${ }M_{4}M_{7}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{1}^{2}$, ${ }M_{3}M_{6}$, ${ }M_{1}M_{7}$, ${ }M_{7}^{2}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{2}M_{6}$, ${ }M_{1}\phi_{1}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{1}M_{3}$, ${ }M_{2}M_{4}$, ${ }M_{3}M_{7}$, ${ }\phi_{1}^{4}$, ${ }M_{1}M_{2}$, ${ }M_{2}M_{7}$, ${ }M_{3}\phi_{1}^{2}$ | ${}$ | -2 | t^2.529 + t^2.647 + 2*t^2.765 + t^2.882 + t^3. + t^3.118 + t^4.088 + t^4.206 + 2*t^4.323 + t^4.441 + t^4.559 + t^4.677 + t^4.794 + t^4.912 + t^5.059 + t^5.176 + t^5.265 + 3*t^5.294 + 2*t^5.412 + 4*t^5.529 + 3*t^5.647 + 3*t^5.765 + t^5.882 - 2*t^6. - t^6.118 - t^6.235 - t^6.353 - t^6.471 - t^6.588 + t^6.617 + 2*t^6.735 + 4*t^6.853 + 5*t^6.97 + 6*t^7.088 + 5*t^7.206 + 4*t^7.323 + 2*t^7.441 + t^7.559 + t^7.588 + t^7.705 + 3*t^7.823 + 3*t^7.941 + 5*t^8.059 + 6*t^8.176 + 7*t^8.294 + 6*t^8.412 + 2*t^8.529 - 4*t^8.765 - 4*t^8.882 - t^4.441/y - t^6.97/y - t^7.088/y - t^7.206/y + t^7.677/y + t^7.794/y + t^7.912/y + t^8.176/y + (2*t^8.294)/y + (3*t^8.412)/y + (3*t^8.529)/y + (4*t^8.647)/y + (3*t^8.765)/y + (3*t^8.882)/y - t^4.441*y - t^6.97*y - t^7.088*y - t^7.206*y + t^7.677*y + t^7.794*y + t^7.912*y + t^8.176*y + 2*t^8.294*y + 3*t^8.412*y + 3*t^8.529*y + 4*t^8.647*y + 3*t^8.765*y + 3*t^8.882*y | g1^8*t^2.529 + g1^6*t^2.647 + 2*g1^4*t^2.765 + g1^2*t^2.882 + t^3. + t^3.118/g1^2 + g1^7*t^4.088 + g1^5*t^4.206 + 2*g1^3*t^4.323 + g1*t^4.441 + t^4.559/g1 + t^4.677/g1^3 + t^4.794/g1^5 + t^4.912/g1^7 + g1^16*t^5.059 + g1^14*t^5.176 + t^5.265/g1^13 + 3*g1^12*t^5.294 + 2*g1^10*t^5.412 + 4*g1^8*t^5.529 + 3*g1^6*t^5.647 + 3*g1^4*t^5.765 + g1^2*t^5.882 - 2*t^6. - t^6.118/g1^2 - t^6.235/g1^4 - t^6.353/g1^6 - t^6.471/g1^8 - t^6.588/g1^10 + g1^15*t^6.617 + 2*g1^13*t^6.735 + 4*g1^11*t^6.853 + 5*g1^9*t^6.97 + 6*g1^7*t^7.088 + 5*g1^5*t^7.206 + 4*g1^3*t^7.323 + 2*g1*t^7.441 + t^7.559/g1 + g1^24*t^7.588 + g1^22*t^7.705 + 3*g1^20*t^7.823 + 3*g1^18*t^7.941 + 5*g1^16*t^8.059 + 6*g1^14*t^8.176 + 7*g1^12*t^8.294 + 6*g1^10*t^8.412 + 2*g1^8*t^8.529 - 4*g1^4*t^8.765 - 4*g1^2*t^8.882 - (g1*t^4.441)/y - (g1^9*t^6.97)/y - (g1^7*t^7.088)/y - (g1^5*t^7.206)/y + t^7.677/(g1^3*y) + t^7.794/(g1^5*y) + t^7.912/(g1^7*y) + (g1^14*t^8.176)/y + (2*g1^12*t^8.294)/y + (3*g1^10*t^8.412)/y + (3*g1^8*t^8.529)/y + (4*g1^6*t^8.647)/y + (3*g1^4*t^8.765)/y + (3*g1^2*t^8.882)/y - g1*t^4.441*y - g1^9*t^6.97*y - g1^7*t^7.088*y - g1^5*t^7.206*y + (t^7.677*y)/g1^3 + (t^7.794*y)/g1^5 + (t^7.912*y)/g1^7 + g1^14*t^8.176*y + 2*g1^12*t^8.294*y + 3*g1^10*t^8.412*y + 3*g1^8*t^8.529*y + 4*g1^6*t^8.647*y + 3*g1^4*t^8.765*y + 3*g1^2*t^8.882*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 |
|---|---|---|---|---|---|---|---|---|---|
| 55090 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{3}^{2}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{1}M_{5}$ | 0.7054 | 0.8688 | 0.8119 | [M:[0.9348, 1.0326, 1.0, 0.9023, 1.0652, 0.8697], q:[0.4511, 0.614], qb:[0.5163, 0.4837], phi:[0.4837]] | t^2.609 + t^2.707 + t^2.805 + t^2.902 + t^3. + t^3.098 + t^3.195 + t^4.158 + t^4.256 + 2*t^4.353 + t^4.451 + t^4.549 + t^4.647 + t^4.744 + t^4.842 + t^5.135 + t^5.218 + t^5.316 + 2*t^5.414 + t^5.511 + 2*t^5.609 + 2*t^5.707 + 3*t^5.805 + t^5.902 - t^6. - t^4.451/y - t^4.451*y | detail |