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 |
|---|---|---|---|---|---|---|---|---|---|
| 58849 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{3}^{2}$ + ${ }M_{1}M_{2}$ + ${ }M_{2}M_{7}$ + ${ }M_{1}M_{5}$ + ${ }M_{1}M_{8}$ | 0.702 | 0.8637 | 0.8128 | [M:[0.9505, 1.0495, 1.0, 0.901, 1.0495, 0.901, 0.9505, 1.0495], q:[0.4505, 0.599], qb:[0.5, 0.5], phi:[0.4876]] | [M:[[-4], [4], [0], [-8], [4], [-8], [-4], [4]], q:[[-4], [8]], qb:[[0], [0]], phi:[[-1]]] | 1 |
| Relevant Operators | Marginal Operators | $n_{marginal}$$-$$|F_{IR}|$ | Superconformal Index | Refined index |
|---|---|---|---|---|
| ${}M_{4}$, ${ }M_{6}$, ${ }M_{7}$, ${ }\phi_{1}^{2}$, ${ }M_{3}$, ${ }M_{5}$, ${ }M_{8}$, ${ }\phi_{1}q_{1}^{2}$, ${ }\phi_{1}q_{1}\tilde{q}_{1}$, ${ }\phi_{1}q_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{1}^{2}$, ${ }\phi_{1}\tilde{q}_{1}\tilde{q}_{2}$, ${ }\phi_{1}\tilde{q}_{2}^{2}$, ${ }\phi_{1}q_{1}q_{2}$, ${ }\phi_{1}q_{2}\tilde{q}_{1}$, ${ }\phi_{1}q_{2}\tilde{q}_{2}$, ${ }\phi_{1}q_{2}^{2}$, ${ }M_{4}^{2}$, ${ }M_{4}M_{6}$, ${ }M_{6}^{2}$, ${ }M_{4}M_{7}$, ${ }M_{6}M_{7}$, ${ }M_{4}\phi_{1}^{2}$, ${ }M_{6}\phi_{1}^{2}$, ${ }M_{3}M_{4}$, ${ }M_{3}M_{6}$, ${ }M_{7}^{2}$, ${ }M_{7}\phi_{1}^{2}$, ${ }M_{4}M_{5}$, ${ }M_{5}M_{6}$, ${ }M_{3}M_{7}$, ${ }M_{4}M_{8}$, ${ }M_{6}M_{8}$, ${ }\phi_{1}^{4}$, ${ }M_{3}\phi_{1}^{2}$ | ${}M_{5}M_{7}$, ${ }M_{7}M_{8}$ | -3 | 2*t^2.703 + t^2.851 + t^2.926 + t^3. + 2*t^3.149 + t^4.166 + 2*t^4.314 + 3*t^4.463 + t^4.611 + 2*t^4.76 + t^5.057 + 3*t^5.406 + t^5.554 + 2*t^5.629 + t^5.703 + t^5.777 + 4*t^5.851 + t^5.926 - 3*t^6. + 2*t^6.074 - t^6.149 + t^6.297 - t^6.446 + 2*t^6.869 + 4*t^7.017 + t^7.092 + 6*t^7.166 + t^7.24 + 5*t^7.314 + t^7.389 + 5*t^7.463 - 2*t^7.537 + 2*t^7.611 + t^7.686 + 2*t^7.76 - 2*t^7.834 + 2*t^7.908 + t^7.983 + 4*t^8.109 - t^8.131 + 2*t^8.206 + t^8.257 + 4*t^8.332 + t^8.406 + 3*t^8.48 + 5*t^8.554 + 4*t^8.629 - 8*t^8.703 + 9*t^8.777 - 7*t^8.851 + 4*t^8.926 - t^4.463/y - (2*t^7.166)/y + t^7.314/y - t^7.389/y + t^7.537/y - t^7.611/y + (2*t^7.76)/y + t^8.406/y + (2*t^8.554)/y + (2*t^8.629)/y + (2*t^8.703)/y + t^8.777/y + (5*t^8.851)/y + t^8.926/y - t^4.463*y - 2*t^7.166*y + t^7.314*y - t^7.389*y + t^7.537*y - t^7.611*y + 2*t^7.76*y + t^8.406*y + 2*t^8.554*y + 2*t^8.629*y + 2*t^8.703*y + t^8.777*y + 5*t^8.851*y + t^8.926*y | (2*t^2.703)/g1^8 + t^2.851/g1^4 + t^2.926/g1^2 + t^3. + 2*g1^4*t^3.149 + t^4.166/g1^9 + (2*t^4.314)/g1^5 + (3*t^4.463)/g1 + g1^3*t^4.611 + 2*g1^7*t^4.76 + g1^15*t^5.057 + (3*t^5.406)/g1^16 + t^5.554/g1^12 + (2*t^5.629)/g1^10 + t^5.703/g1^8 + t^5.777/g1^6 + (4*t^5.851)/g1^4 + t^5.926/g1^2 - 3*t^6. + 2*g1^2*t^6.074 - g1^4*t^6.149 + g1^8*t^6.297 - g1^12*t^6.446 + (2*t^6.869)/g1^17 + (4*t^7.017)/g1^13 + t^7.092/g1^11 + (6*t^7.166)/g1^9 + t^7.24/g1^7 + (5*t^7.314)/g1^5 + t^7.389/g1^3 + (5*t^7.463)/g1 - 2*g1*t^7.537 + 2*g1^3*t^7.611 + g1^5*t^7.686 + 2*g1^7*t^7.76 - 2*g1^9*t^7.834 + 2*g1^11*t^7.908 + g1^13*t^7.983 + (4*t^8.109)/g1^24 - g1^17*t^8.131 + 2*g1^19*t^8.206 + t^8.257/g1^20 + (4*t^8.332)/g1^18 + t^8.406/g1^16 + (3*t^8.48)/g1^14 + (5*t^8.554)/g1^12 + (4*t^8.629)/g1^10 - (8*t^8.703)/g1^8 + (9*t^8.777)/g1^6 - (7*t^8.851)/g1^4 + (4*t^8.926)/g1^2 - t^4.463/(g1*y) - (2*t^7.166)/(g1^9*y) + t^7.314/(g1^5*y) - t^7.389/(g1^3*y) + (g1*t^7.537)/y - (g1^3*t^7.611)/y + (2*g1^7*t^7.76)/y + t^8.406/(g1^16*y) + (2*t^8.554)/(g1^12*y) + (2*t^8.629)/(g1^10*y) + (2*t^8.703)/(g1^8*y) + t^8.777/(g1^6*y) + (5*t^8.851)/(g1^4*y) + t^8.926/(g1^2*y) - (t^4.463*y)/g1 - (2*t^7.166*y)/g1^9 + (t^7.314*y)/g1^5 - (t^7.389*y)/g1^3 + g1*t^7.537*y - g1^3*t^7.611*y + 2*g1^7*t^7.76*y + (t^8.406*y)/g1^16 + (2*t^8.554*y)/g1^12 + (2*t^8.629*y)/g1^10 + (2*t^8.703*y)/g1^8 + (t^8.777*y)/g1^6 + (5*t^8.851*y)/g1^4 + (t^8.926*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 |
|---|---|---|---|---|---|---|---|---|---|
| 56965 | SU2adj1nf2 | ${}M_{1}q_{1}q_{2}$ + ${ }M_{2}q_{1}\tilde{q}_{1}$ + ${ }M_{3}\tilde{q}_{1}\tilde{q}_{2}$ + ${ }M_{4}q_{2}\tilde{q}_{2}$ + ${ }M_{5}q_{1}\tilde{q}_{2}$ + ${ }M_{6}q_{2}\tilde{q}_{1}$ + ${ }M_{3}^{2}$ + ${ }M_{1}M_{2}$ + ${ }M_{2}M_{7}$ + ${ }M_{1}M_{5}$ | 0.7071 | 0.8737 | 0.8094 | [M:[0.9401, 1.0599, 1.0, 0.8801, 1.0599, 0.8801, 0.9401], q:[0.4401, 0.6199], qb:[0.5, 0.5], phi:[0.485]] | 2*t^2.64 + 2*t^2.82 + t^2.91 + t^3. + t^3.18 + t^4.095 + 2*t^4.275 + 3*t^4.455 + t^4.635 + 2*t^4.815 + t^5.174 + 3*t^5.281 + 3*t^5.46 + 2*t^5.55 + 3*t^5.64 + 2*t^5.73 + 3*t^5.82 + t^5.91 - 3*t^6. - t^4.455/y - t^4.455*y | detail |