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 |
|---|---|---|---|---|---|---|---|---|---|
| 4533 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{7}$ + ${ }M_{1}M_{8}$ | 0.6972 | 0.855 | 0.8154 | [M:[0.9487, 1.0171, 1.0513, 0.9145, 1.0, 0.9658, 0.9829, 1.0513], q:[0.5, 0.5513], qb:[0.4487, 0.5342], phi:[0.4914]] | [M:[[-6], [2], [6], [-10], [0], [-4], [-2], [6]], q:[[0], [6]], qb:[[-6], [4]], phi:[[-1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }M_{6}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{5}$, ${ }M_{3}$, ${ }M_{8}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{4}M_{7}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{6}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{5}M_{6}$, ${ }M_{7}^{2}$, ${ }M_{4}M_{8}$, ${ }M_{7}\phi_{1}^{2}$, ${ }\phi_{1}^{4}$, ${ }M_{5}M_{7}$, ${ }M_{5}\phi_{1}^{2}$ | ${}$ | -3 | t^2.743 + t^2.897 + 2*t^2.949 + t^3. + 2*t^3.154 + t^4.167 + t^4.32 + t^4.423 + 2*t^4.474 + t^4.577 + t^4.628 + t^4.68 + t^4.731 + t^4.782 + t^5.487 + t^5.641 + t^5.692 + t^5.795 + 5*t^5.897 + t^5.949 - 3*t^6. + t^6.051 + 2*t^6.103 - t^6.257 + 2*t^6.308 + t^6.91 + 2*t^7.064 + 2*t^7.115 + t^7.167 + t^7.218 + t^7.269 + 2*t^7.32 + 3*t^7.372 + 3*t^7.423 + t^7.474 + 2*t^7.577 + 4*t^7.628 + 2*t^7.68 + t^7.731 + t^7.782 + t^7.885 + 2*t^7.936 + t^8.23 + t^8.333 + t^8.384 + t^8.436 + t^8.487 + t^8.538 + 4*t^8.641 - 2*t^8.743 + 4*t^8.795 + 4*t^8.846 - t^8.897 - 2*t^8.949 - t^4.474/y - t^7.218/y + t^7.32/y - t^7.372/y - t^7.423/y + t^7.526/y + t^7.577/y - t^7.628/y + t^7.731/y + t^8.641/y + (2*t^8.692)/y + t^8.743/y + (2*t^8.846)/y + (4*t^8.897)/y + (2*t^8.949)/y - t^4.474*y - t^7.218*y + t^7.32*y - t^7.372*y - t^7.423*y + t^7.526*y + t^7.577*y - t^7.628*y + t^7.731*y + t^8.641*y + 2*t^8.692*y + t^8.743*y + 2*t^8.846*y + 4*t^8.897*y + 2*t^8.949*y | t^2.743/g1^10 + t^2.897/g1^4 + (2*t^2.949)/g1^2 + t^3. + 2*g1^6*t^3.154 + t^4.167/g1^13 + t^4.32/g1^7 + t^4.423/g1^3 + (2*t^4.474)/g1 + g1^3*t^4.577 + g1^5*t^4.628 + g1^7*t^4.68 + g1^9*t^4.731 + g1^11*t^4.782 + t^5.487/g1^20 + t^5.641/g1^14 + t^5.692/g1^12 + t^5.795/g1^8 + (5*t^5.897)/g1^4 + t^5.949/g1^2 - 3*t^6. + g1^2*t^6.051 + 2*g1^4*t^6.103 - g1^10*t^6.257 + 2*g1^12*t^6.308 + t^6.91/g1^23 + (2*t^7.064)/g1^17 + (2*t^7.115)/g1^15 + t^7.167/g1^13 + t^7.218/g1^11 + t^7.269/g1^9 + (2*t^7.32)/g1^7 + (3*t^7.372)/g1^5 + (3*t^7.423)/g1^3 + t^7.474/g1 + 2*g1^3*t^7.577 + 4*g1^5*t^7.628 + 2*g1^7*t^7.68 + g1^9*t^7.731 + g1^11*t^7.782 + g1^15*t^7.885 + 2*g1^17*t^7.936 + t^8.23/g1^30 + t^8.333/g1^26 + t^8.384/g1^24 + t^8.436/g1^22 + t^8.487/g1^20 + t^8.538/g1^18 + (4*t^8.641)/g1^14 - (2*t^8.743)/g1^10 + (4*t^8.795)/g1^8 + (4*t^8.846)/g1^6 - t^8.897/g1^4 - (2*t^8.949)/g1^2 - t^4.474/(g1*y) - t^7.218/(g1^11*y) + t^7.32/(g1^7*y) - t^7.372/(g1^5*y) - t^7.423/(g1^3*y) + (g1*t^7.526)/y + (g1^3*t^7.577)/y - (g1^5*t^7.628)/y + (g1^9*t^7.731)/y + t^8.641/(g1^14*y) + (2*t^8.692)/(g1^12*y) + t^8.743/(g1^10*y) + (2*t^8.846)/(g1^6*y) + (4*t^8.897)/(g1^4*y) + (2*t^8.949)/(g1^2*y) - (t^4.474*y)/g1 - (t^7.218*y)/g1^11 + (t^7.32*y)/g1^7 - (t^7.372*y)/g1^5 - (t^7.423*y)/g1^3 + g1*t^7.526*y + g1^3*t^7.577*y - g1^5*t^7.628*y + g1^9*t^7.731*y + (t^8.641*y)/g1^14 + (2*t^8.692*y)/g1^12 + (t^8.743*y)/g1^10 + (2*t^8.846*y)/g1^6 + (4*t^8.897*y)/g1^4 + (2*t^8.949*y)/g1^2 |
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 |
|---|---|---|---|---|---|---|---|---|---|
| 2481 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{3}q_{1}\tilde{q}_{1}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{2}\tilde{q}_{1}$ + ${ }M_{5}^{2}$ + ${ }M_{1}M_{3}$ + ${ }M_{2}\phi_{1}^{2}$ + ${ }M_{6}q_{1}\tilde{q}_{2}$ + ${ }M_{2}M_{7}$ | 0.7029 | 0.8658 | 0.8118 | [M:[0.929, 1.0237, 1.071, 0.8816, 1.0, 0.9527, 0.9763], q:[0.5, 0.571], qb:[0.429, 0.5473], phi:[0.4882]] | t^2.645 + t^2.787 + t^2.858 + 2*t^2.929 + t^3. + t^3.213 + t^4.038 + t^4.251 + t^4.393 + 2*t^4.464 + t^4.607 + t^4.678 + t^4.749 + t^4.82 + t^4.891 + t^5.29 + t^5.432 + t^5.503 + 2*t^5.574 + t^5.645 + 3*t^5.716 + t^5.787 + 4*t^5.858 + t^5.929 - 2*t^6. - t^4.464/y - t^4.464*y | detail |